Method for neutral beam processing based on gas cluster ion beam technology and articles produced thereby

ABSTRACT

A method for treating a silicon substrate, and a silicon substrate, provide a surface treated with an accelerated neutral beam.

FIELD OF THE INVENTION

This invention relates generally to methods and apparatus for low energy, Neutral Beam processing and more specifically to high beam purity methods and systems for deriving an accelerated neutral monomer and/or neutral gas cluster beam from an accelerated gas cluster ion beam. The invention also includes certain new or improved materials and devices made by the materials.

BACKGROUND OF THE INVENTION

During the past decade, the gas cluster ion beam (GCIB) has become well known and widely used for a variety of surface and subsurface processing applications. Because gas cluster ions typically have a large mass, they tend to travel at relatively low velocities (compared to conventional ions) even when accelerated to substantial energies. These low velocities, combined with the inherently weak binding of the clusters, result in unique surface processing capabilities that lead to reduced surface penetration and reduced surface damage compared to conventional ion beams and diffuse plasmas.

Gas cluster ion beams have been employed to smooth, etch, clean, form deposits on, grow films on, or otherwise modify a wide variety of surfaces including for example, metals, semiconductors, and dielectric materials. In applications involving semiconductor and semiconductor-related materials, GCIBs have been employed to clean, smooth, etch, deposit and/or grow films including oxides and others. GCIBs have also been used to introduce doping and lattice-straining atomic species, materials for amorphizing surface layers, and to improve dopant solubility in semiconductor materials. In many cases such GCIB applications have been able to provide results superior to other technologies that employ conventional ions, ion beams, and plasmas. Semiconductor materials include a wide range of materials that may have their electrical properties manipulated by the introduction of dopant materials, and include (without limitation) silicon, germanium, diamond, silicon carbide, and also compound materials comprising group III-IV elements, and group II-VI elements. Because of the ease of forming GCIBs using argon (Ar) as a source gas and because of the inert properties of argon, many applications have been developed for processing the surfaces of implantable medical devices such as coronary stents, orthopedic prostheses, and other implantable medical devices using argon gas GCIBs. In semiconductor applications, a variety of source gases and source gas mixtures have been employed to form GCIBs containing electrical dopants and lattice-straining species, for reactive etching, physical etching, film deposition, film growth, and other useful processes. A variety of practical systems for introducing GCIB processing to a wide range of surface types are known. For example, U.S. Pat. No. 6,676,989 C1 issued to Kirkpatrick et al. teaches a GCIB processing system having a workpiece holder and manipulator suited for processing tubular or cylindrical workpieces such as vascular stents. In another example, U.S. Pat. No. 6,491,800 B2 issued to Kirkpatrick et al. teaches a GCIB processing system having workpiece holders and manipulators for processing other types of non-planar medical devices, including for example, hip joint prostheses. A further example, U.S. Pat. No. 6,486,478 B1 issued to Libby et al. teaches an automated substrate loading/unloading system suitable for processing semiconductor wafers. U.S. Pat. No. 7,115,511 issued to Hautala, teaches the use of a mechanical scanner for scanning a workpiece relative to an un-scanned GCIB. In still another example, U.S. Pat. No. 7,105,199 B2 issued to Blinn et al. teaches the use of GCIB processing to improve the adhesion of drug coatings on medical devices and to modify the elution or release rate of a drug from the medical devices.

GCIB has been employed in etching and smoothing of crystalline and non-crystalline forms of materials such as diamonds and other gemstones. This has not been entirely successful in that at times the gemstone may undergo undesirable color changes as a result of the GCIB processing. It has not been clear whether this results from some form of surface or sub-surface damage to the gemstone materials, or might be due to the formation of a roughened interface between the etched and/or smoothed surface layer resulting from the GCIB processing and the underlying unmodified bulk of the material, or is perhaps due to damage due to surface electrical charging induced by the cluster ions. Whatever the cause of the negative side effects of the GCIB processing, a processing technique for etching and/or smoothing of natural and synthetic gemstone materials that does not introduce undesired degradation of the appearance and esthetic appeal of the gems is desirable. GCIB processing has been indicated as a possible technique for smoothing and/or planarizing surfaces of optical materials such as lenses, reflecting optical surfaces, optical windows, optical panels for display and touch-screen panels, prismatic devices, transparent substrates for photo-masks and the like, optical waveguides, electro-optical devices, and other optical devices. Materials for optical devices include a wide variety of glasses, quartz, sapphire, diamond, and other hard, transparent materials. Conventional polishing and planarizing including mechanical, chemical-mechanical, and other techniques have not produced adequate surfaces for the most demanding applications. GCIB processing has in many cases been shown to be capable of smoothing and/or planarizing optical surfaces to a degree not obtainable by conventional polishing techniques, but alternative techniques that do not result in a rough interface between the smoothed surface and the underlying bulk material are needed to avoid creation of scattering layers embedded in the optical material.

Although GCIB processing has been employed successfully for many applications, there are new and existing application needs not fully met by GCIB or other state of the art methods and apparatus. In many situations, while a GCIB can produce dramatic atomic-scale smoothing of an initially somewhat rough surface, the ultimate smoothing that can be achieved is often less than the required smoothness, and in other situations GCIB processing can result in roughening moderately smooth surfaces rather than smoothing them further.

Other needs/opportunities also exist as recognized and resolved through embodiments of the present invention. In the field of drug-eluting medical implants, GCIB processing has been successful in treating surfaces of drug coatings on medical implants to bind the coating to a substrate or to modify the rate at which drugs are eluted from the coating following implantation into a patient. However, it has been noted that in some cases where GCIB has been used to process drug coatings (which are often very thin and may comprise very expensive drugs), there may occur a weight loss of the drug coating (indicative of drug loss or removal) as a result of the GCIB processing. For the particular cases where such loss occurs (certain drugs and using certain processing parameters) the occurrence is generally undesirable and having a process with the ability to avoid the weight loss, while still obtaining satisfactory control of the drug elution rate, is preferable.

In semiconductor applications, GCIBs have been employed with varying degrees of success in many surface-processing improvements, however opportunities for improvement exist. In conventional GCIB processing, often the result, though significantly improved over earlier conventional technologies, is still not of the quality that is required by the most demanding applications. For example, in smoothing processes, for many materials the final degree of smoothness practically obtainable using GCIB processing does not always meet requirements. In applications where other materials are introduced into semiconductor materials (sometimes called GCIB infusion) for purposes of doping, lattice-straining, and other applications such as film deposition, film growth, and amorphization, the interface between the infused, grown, amorphized, or deposited material often has a roughness or non-uniformity at the interface between the irradiated layer and the underlying substrate that impairs optimal performance of the GCIB-modified layer.

Ions have long been favored for many processes because their electric charge facilitates their manipulation by electrostatic and magnetic fields. This introduces great flexibility in processing. However, in some applications, the charge that is inherent to any ion (including gas cluster ions in a GCIB) may produce undesirable effects in the processed surfaces. GCIB has a distinct advantage over conventional ion beams in that a gas cluster ion with a single or small multiple charge enables the transport and control of a much larger mass-flow (a cluster may consist of hundreds or thousands of molecules) compared to a conventional ion (a single atom, molecule, or molecular fragment.) Particularly in the case of insulating materials, surfaces processed using ions often suffer from charge-induced damage resulting from abrupt discharge of accumulated charges, or production of damaging electrical field-induced stress in the material (again resulting from accumulated charges.) In many such cases, GCIBs have an advantage due to their relatively low charge per mass, but in some instances may not eliminate the target-charging problem. Furthermore, moderate to high current intensity ion beams may suffer from a significant space charge-induced defocusing of the beam that tends to inhibit transporting a well-focused beam over long distances. Again, due to their lower charge per mass relative to conventional ion beams, GCIBs have an advantage, but they do not fully eliminate the space charge transport problem.

A further instance of need or opportunity arises from the fact that although the use of beams of neutral molecules or atoms provides benefit in some surface processing applications and in space charge-free beam transport, it has not generally been easy and economical to produce intense beams of neutral molecules or atoms except for the case of nozzle jets, where the energies are generally on the order of a few milli-electron-volts per atom or molecule, and thus have limited processing capabilities.

In U.S. Pat. No. 4,935,623 of Hughes Electronics Corporation, Knauer has taught a method for forming beams of energetic (1 to 10 eV) charged and/or neutral atoms. Knauer forms a conventional GCIB and directs it at grazing angles against solid surfaces such as silicon plates, which dissociates the cluster ions, resulting in a forward-scattered beam of atoms and conventional ions. This results in an intense but unfocused beam of neutral atoms and ions that may be used for processing, or that following electrostatic separation of the ions may be used for processing as a neutral atom beam. By requiring the scattering of the GCIB off of a solid surface to produce dissociation, a significant problem is introduced by the Knauer techniques. Across a wide range of beam energies, a GCIB produces strong sputtering in surfaces that it strikes. It has been clearly shown (see for example Aoki, T and Matsuo, J, “Molecular dynamics simulations of surface smoothing and sputtering process with glancing-angle gas cluster ion beams,” Nucl. Instr. & Meth. in Phys. Research B 257 (2007), pp. 645-648) that even at grazing angles as employed by Knauer, GCIBs produce considerable sputtering of solids, and thus the forward-scattered neutral beam is contaminated by sputtered ions and neutral atoms and other particles originating in the solid surface used for scattering/dissociation. In a multitude of applications including medical device processing applications and semiconductor processing applications, the presence of such sputtered material contaminating the forward-scattered beam renders it unsuitable for use.

In U.S. Pat. No. 7,060,989, Swenson et al. teach the use of a gas pressure cell having gas pressure higher than the beam generation pressure to modify the gas cluster ion energy distribution in a GCIB. The technique lowers the energy of gas cluster ions in a GCIB and modifies some of the surface processing characteristics of such modified GCIBs. Such gas modification of GCIB gas cluster ion energy distribution is helpful, but does not reduce problems caused by charges deposited in the workpiece by the ions in the GCIB and does not solve certain processing problems, as for example, the weight loss of drug coatings during GCIB processing. Although the techniques of Swenson et al. can improve the ultimate surface smoothing characteristics of a GCIB, the result is still less than ideal.

Gas clusters and gas cluster ion sizes are typically characterized by N, the number of atoms or molecules (depending on whether the gas is atomic or molecular and including variants such as ions, monomers, dimmers, trimers, ligands) comprising the individual cluster. Many of the advantages contributed by conventional GCIB processing are believed to derive from the low velocities of ions in the GCIB and from the fact that large, loosely bound clusters disintegrate on collision with a solid surface, causing transient heating and pressure but without excessive penetration, implantation, or damage to the substrate beneath the surface. Effects of such large clusters (having N monomers—as defined below—on the order of a few thousand or more) are generally limited to a few tens of Angstroms. However, it has been shown that smaller clusters (having N on the order of a few hundred to about a thousand) produce more damage to an impacted surface and are capable of producing discrete impact craters in a surface (see for example, Houzumi, H., et al. “Scanning tunneling microscopy observation of graphite surfaces irradiated with size-selected Ar cluster ion beams”, Jpn. J Appl. Phys. V44(8), (2005), p 6252 ff). This crater-forming effect can roughen and remove material from surfaces (etch) in undesirable competition with the surface smoothing effects of the larger clusters. In many other surface processing applications for which GCIB have been found useful, it is believed that the effects of large gas cluster ions and smaller gas cluster ions may compete in counter-productive ways to reduce processing performance. Unfortunately, the readily applied techniques for forming GCIBs all result in generation of beams having a broad distribution of cluster sizes having size, N, ranging from around 100 to as much as several tens of thousands. Often the mean and/or peak of the size distribution lies in the range of from several hundred to a few thousand, with distribution tails gradually diminishing to zero at the size extremes of the distribution. The cluster-ion size distribution and the mean cluster size, N_(Mean), associated with the distribution is dependent on the source gas employed and can be significantly influenced by selection of the parameters of the nozzle used to form the cluster jet, by the pressure drop through the nozzle, and by the nozzle temperature, all according to conventional GCIB formation techniques. Most commercial GCIB processing tools routinely employ magnetic or occasionally electrostatic size separators to remove the smallest ions and clusters (monomers, dimers, trimers, etc. up to around N=10 or more), which are the most damaging. Such filters are often referred to as “monomer filters”, although they typically also remove somewhat larger ions as well as the monomers. Certain electrostatic cluster ion size selectors (as for example the one employed in U.S. Pat. No. 4,935,623, by Knauer) require placing grids of electrical conductors into the beam, which introduces a strong disadvantage due to potential erosion of the grids by the beam, introducing beam contamination while reducing reliability and resulting in the need for additional maintenance to the apparatus. For that reason, monomer and low-mass filters are now typically of the magnetic type (see for examples, U.S. Pat. No. 6,635,883, to Torti et al. and U.S. Pat. No. 6,486,478, to Libby et al.) Aside from the smallest ions (monomers, dimers, etc.), which are effectively removed by magnetic filters, it appears that most GCIBs contain few or no gas cluster ions of sizes below about N=100. It may be that such sizes do not readily form or after forming are not stable. However, clusters in the range from about N=100 to a few hundred seem to be present in the beams of most commercial GCIB processing tools. Values of N_(Mean) in the range of from a few hundred to several thousand are commonly encountered when using conventional techniques. Because, for a given acceleration potential the intermediate size clusters travel much faster than the larger clusters, they are more likely to produce craters, rough interfaces, and other undesirable effects, and probably contribute to less than ideal processing when present in a GCIB.

It is therefore an object of this invention to provide apparatus and methods for forming high purity neutral gas cluster beams for workpiece processing.

It is a further object of this invention to provide apparatus and methods to provide high purity gas cluster beams that are substantially free of intermediate size clusters.

Yet another object of this invention is to provide apparatus and methods for forming high purity, focused, intense beams of neutral atoms or molecules with energies in the range of from about 1 eV to as much as a few thousand eV.

Still another object of this invention is to provide apparatus and methods for forming beams capable of improved surface smoothing compared to conventional GCIBs.

An object of this invention is to provide apparatus and methods for forming doped and/or strained films and/or for introducing foreign atomic species into the surfaces of semiconductor or other materials, wherein the processed surface have interfaces to the underlying substrate material that are superior to those formed using conventional GCIB processing.

Another object of this invention is to provide apparatus and methods for forming amorphous regions at the surface of a semiconductor or other material using a Neutral Beam and wherein the interface to the underlying substrate material is superior to one formed using conventional GCIB processing.

A further object of this invention is to provide apparatus and methods for etching surfaces with superior final smoothness as compared to conventional GCIB processing.

A still further object of this invention is to provide apparatus and methods for etching optical surfaces with superior final smoothness as compared to conventional GCIB processing.

Another object of this invention is to provide apparatus and methods for adhering an optical coating to an optical surface with adhesion superior to that obtained by conventional methods.

Another object of this invention is to provide methods for modifying a surface of an optical device to reduce its susceptibility do degradation due to atmospheric exposure, and to provide optical devices thereby improved.

A further object of this invention is to provide methods for forming a barrier on a surface of a hygroscopic material to reduce the susceptibility of the material to absorption of moisture, and to provide materials thereby improved.

Yet another object of this invention is to provide apparatus and methods for forming and/or growing films on surfaces of semiconductor and/or other materials, having interfaces to the underlying substrate material that are superior to those formed using conventional GCIB processing.

An additional object of this invention is to provide apparatus and methods for treating electrically insulating materials with Neutral Beams of gas clusters and/or monomers for processing such materials without damage induced by beam transported electrical charges.

A further object of this invention is to provide methods for improving properties of an optical element or a gem by Neutral Beam irradiation of a surface of the optical element.

Another object of this invention is to provide an optical element or gem with improved properties by Neutral Beam technology.

An additional object of this invention is to provide a method of forming a SiC or SiC_(x) layer on a silicon substrate

SUMMARY OF THE INVENTION

The objects set forth above as well as further and other objects and advantages of the present invention are achieved by the various embodiments of the invention described herein below.

One embodiment of the present invention provides a method of treating a surface of a silicon substrate comprising the steps of: providing a reduced pressure chamber; forming a gas cluster ion beam, comprising gas cluster ions comprising carbon atoms, within the reduced pressure chamber; accelerating the gas cluster ions to form an accelerated gas cluster ion beam along a beam path within the reduced pressure chamber; promoting fragmentation and/or dissociation of at least a portion of the accelerated gas cluster ions along the beam path; removing charged particles from the beam path to form an accelerated neutral beam along the beam path in the reduced pressure chamber; holding the silicon substrate in the beam path; treating at least a portion of a surface of the silicon substrate by irradiating it with the accelerated neutral beam; and wherein the promoting and removing steps occur prior to irradiating the surface.

The step of removing may remove essentially all charged particles from the beam path. The neutral beam may be substantially free of intermediate sized clusters. The neutral beam may consist essentially of gas from the gas cluster ion beam. The step of promoting may include raising an acceleration voltage in the step of accelerating or improving ionization efficiency in the forming of the gas cluster ion beam. The step of promoting may include increasing the range of velocities of ions in the accelerated gas cluster ion beam. The step of promoting may include introducing one or more gaseous elements used in forming the gas cluster ion beam into the reduced pressure chamber to increase pressure along the beam path. The step of promoting may include increasing the size of a skimmer aperture used in the step of forming the gas cluster ion beam. The step of promoting may include irradiating the accelerated gas cluster ion beam or the neutral beam with radiant energy. The neutral beam treating at least a portion of a surface of the workpiece may consist substantially of monomers having an energy between 1 eV and several thousand eV. The method may further comprise the step of repositioning the workpiece with a workpiece holder to treat plural portions of the surface. The method may further comprise the step of scanning the workpiece with a workpiece holder to treat extended portions of the surface.

The silicon substrate may comprise any of a crystalline material or an amorphous

The method may further comprise the step of heat treating the irradiated silicon substrate to anneal it or to restore crystallinity to the treated substrate or to move the implanted carbon to lattice substitutional sites in the silicon substrate.

The treating step may modify a surface property of the silicon substrate. The surface property may be modified to be harder, more heat resistant, less damage prone, more refractory, have improved chemical properties, or to have a different lattice constant. The modified surface property may be modified to be better suited to serve as a base for subsequent layer growth or to serve as a substrate for deposition of subsequent material.

Another embodiment of the present invention provides a silicon substrate having a surface layer of SiC_(x) (0.05<X<3) formed by accelerated Neutral Beam irradiation of a silicon substrate.

The present invention provides a high beam purity method and system for deriving from an accelerated gas cluster ion beam an accelerated neutral gas cluster and/or preferably monomer beam that can be employed for a variety of types of surface and shallow subsurface materials processing and which is capable, for many applications, of superior performance compared to conventional GCIB processing. It can provide well-focused, accelerated, intense neutral monomer beams with particles having energies in the range of from about 1 eV to as much as a few thousand eV. In this energy range neutral particles can be beneficial or necessary in many applications, for example when it is desirable to break surface or shallow subsurface bonds to facilitate cleaning, etching, smoothing, deposition, amorphization, or to produce surface chemistry effects. In such cases, energies of from about an eV up to a few thousands of eV per particle can often be useful. This is an energy range in which it has been impractical with simple, relatively inexpensive apparatus to form intense neutral beams. In various embodiments, the accelerated Neutral Beam is employed for a variety of surface and shallow subsurface materials processing and to make enhanced materials and devices by such processing methods.

These accelerated Neutral Beams are generated by first forming a conventional accelerated GCIB, then partly or essentially fully dissociating it by methods and operating conditions that do not introduce impurities into the beam, then separating the remaining charged portions of the beam from the neutral portion, and subsequently using the resulting accelerated Neutral Beam for workpiece processing. Depending on the degree of dissociation of the gas cluster ions, the Neutral Beam produced may be a mixture of neutral gas monomers and gas clusters or may essentially consist entirely or almost entirely of neutral gas monomers. It is preferred that the accelerated Neutral Beam is an essentially fully dissociated neutral monomer beam.

An advantage of the Neutral Beams that may be produced by the methods and apparatus of the embodiments of this invention, is that they may be used to process electrically insulating materials without producing damage to the material due to charging of the surfaces of such materials by beam transported charges as commonly occurs for all ionized beams including GCIB. For example, in semiconductor and other electronic applications, ions often contribute to damaging or destructive charging of thin dielectric films such as oxides, nitrides, etc. The use of Neutral Beams can enable successful beam processing of polymer, dielectric, and/or other electrically insulating or high resistivity materials, coatings, and films in other applications where ion beams may produce unacceptable side effects due to surface charging or other charging effects. Examples include (without limitation) processing of corrosion inhibiting coatings, and irradiation cross-linking and/or polymerization of organic films. In other examples, Neutral Beam induced modifications of polymer or other dielectric materials (e.g. sterilization, smoothing, improving surface biocompatibility, and improving attachment of and/or control of elution rates of drugs) may enable the use of such materials in medical devices for implant and/or other medical/surgical applications. Further examples include Neutral Beam processing of glass, polymer, and ceramic bio-culture labware and/or environmental sampling surfaces where such beams may be used to improve surface characteristics like, for example, roughness, smoothness, hydrophilicity, and biocompatibility.

Since the parent GCIB, from which accelerated Neutral Beams may be formed by the methods and apparatus of embodiments of the invention, comprises ions, it is readily accelerated to desired energy and is readily focused using conventional ion beam techniques. Upon subsequent dissociation and separation of the charged ions from the neutral particles, the Neutral Beam particles tend to retain their focused trajectories and may be transported for extensive distances with good effect.

When neutral gas clusters in a jet are ionized by electron bombardment, they become heated and/or excited. This may result in subsequent evaporation of monomers from the ionized gas cluster, after acceleration, as it travels down the beamline. Additionally, collisions of gas cluster ions with background gas molecules in the ionizer, accelerator and beamline regions, also heat and excite the gas cluster ions and may result in additional subsequent evolution of monomers from the gas cluster ions following acceleration. When these mechanisms for evolution of monomers are induced by electron bombardment and/or collision with background gas molecules (and/or other gas clusters) of the same gas from which the GCIB was formed, no contamination is contributed to the beam by the dissociation processes that results in evolving the monomers.

There are other mechanisms that can be employed for dissociating (or inducing evolution of monomers from) gas cluster ions in a GCIB without introducing contamination into the beam. Some of these mechanisms may also be employed to dissociate neutral gas clusters in a neutral gas cluster beam. One mechanism is laser irradiation of the cluster-ion beam using infra-red or other laser energy. Laser-induced heating of the gas cluster ions in the laser irradiated GCIB results in excitement and/or heating of the gas cluster ions and causes subsequent evolution of monomers from the beam. Another mechanism is passing the beam through a thermally heated tube so that radiant thermal energy photons impact the gas cluster ions in beam. The induced heating of the gas cluster ions by the radiant thermal energy in the tube results in excitement and/or heating of the gas cluster ions and causes subsequent evolution of monomers from the beam. In another mechanism, crossing the gas cluster ion beam by a gas jet of the same gas or mixture as the source gas used in formation of the GCIB (or other non-contaminating gas) results in collisions of monomers of the gas in the gas jet with the gas clusters in the ion beam producing excitement and/or heating of the gas cluster ions in the beam and subsequent evolution of monomers from the excited gas cluster ions. By depending entirely on electron bombardment during initial ionization and/or collisions (with other cluster ions, or with background gas molecules of the same gas(es) as those used to form the GCIB) within the beam and/or laser or thermal radiation and/or crossed jet collisions of non-contaminating gas to produce the GCIB dissociation and/or fragmentation, contamination of the beam by collision with other materials is avoided.

Through the use of such non-contaminating methods of dissociation described above, the GCIB is dissociated or at least partially dissociated without introducing atoms to the dissociation products or residual clusters that are not part of the original source gas atoms. By using a source gas for initial cluster formation that does not contain atoms which would be contaminants for the workpiece to be processed using the residual clusters or dissociation products, contamination of the workpiece is avoided. When argon or other noble gases are employed, the source gas materials are volatile and not chemically reactive, and upon subsequent irradiation of the workpiece using Neutral Beams these volatile non-reactive atoms are fully released from the workpiece. Thus for workpieces that are optical and gem materials including glasses, quartz, sapphire, diamond, and other hard, transparent materials such as lithium triborate (LBO), argon and other noble gases can serve as source gas materials without contributing contamination due to Neutral Beam irradiation. In other cases, other source gases may be employed, provided the source gas atomic constituents do not include atoms that would result in contamination of the workpiece. For example, for some glass workpieces, LBO, and various other optical materials are oxygen containing, and oxygen atoms may not serve as contaminants. In such cases oxygen-containing source gases may be employed without contamination.

As a neutral gas cluster jet from a nozzle travels through an ionizing region where electrons are directed to ionize the clusters, a cluster may remain un-ionized or may acquire a charge state, q, of one or more charges (by ejection of electrons from the cluster by an incident electron). The ionizer operating conditions influence the likelihood that a gas cluster will take on a particular charge state, with more intense ionizer conditions resulting in greater probability that a higher charge state will be achieved. More intense ionizer conditions resulting in higher ionization efficiency may result from higher electron flux and/or higher (within limits) electron energy. Once the gas cluster has been ionized, it is typically extracted from the ionizer, focused into a beam, and accelerated by falling through an electric field. The amount of acceleration of the gas cluster ion is readily controlled by controlling the magnitude of the accelerating electric field. Typical commercial GCIB processing tools generally provide for the gas cluster ions to be accelerated by an electric field having an adjustable accelerating potential, V_(Acc), typically of, for example, from about 1 kV to 70 kV (but not limited to that range—V_(Acc) up to 200 kV or even more may be feasible). Thus a singly charged gas cluster ion achieves an energy in the range of from 1 to 70 keV (or more if larger V_(Acc) is used) and a multiply charged (for example, without limitation, charge state, q=3 electronic charges) gas cluster ion achieves an energy in the range of from 3 to 210 keV (or more for higher V_(Acc)). For other gas cluster ion charge states and acceleration potentials, the accelerated energy per cluster is qV_(Acc) eV. From a given ionizer with a given ionization efficiency, gas cluster ions will have a distribution of charge states from zero (not ionized) to a higher number such as for example 6 (or with high ionizer efficiency, even more), and the most probable and mean values of the charge state distribution also increase with increased ionizer efficiency (higher electron flux and/or energy). Higher ionizer efficiency also results in increased numbers of gas cluster ions being formed in the ionizer. In many cases, GCIB processing throughput increases when operating the ionizer at high efficiency results in increased GCIB current. A downside of such operation is that multiple charge states that may occur on intermediate size gas cluster ions can increase crater and/or rough interface formation by those ions, and often such effects may operate counterproductively to the intent of the processing. Thus for many GCIB surface processing recipes, selection of the ionizer operating parameters tends to involve more considerations than just maximizing beam current. In some processes, use of a “pressure cell” (see U.S. Pat. No. 7,060,989, to Swenson et al.) may be employed to permit operating an ionizer at high ionization efficiency while still obtaining acceptable beam processing performance by moderating the beam energy by gas collisions in an elevated pressure “pressure cell.”

When the Neutral Beams are formed in embodiments of the present invention there is no downside to operating the ionizer at high efficiency—in fact such operation is sometimes preferred. When the ionizer is operated at high efficiency, there may be a wide range of charge states in the gas cluster ions produced by the ionizer. This results in a wide range of velocities in the gas cluster ions in the extraction region between the ionizer and the accelerating electrode, and also in the downstream beam. This may result in an enhanced frequency of collisions between and among gas cluster ions in the beam that generally results in a higher degree of fragmentation of the largest gas cluster ions. Such fragmentation may result in a redistribution of the cluster sizes in the beam, skewing it toward the smaller cluster sizes. These cluster fragments retain energy in proportion to their new size (N) and so become less energetic while essentially retaining the accelerated velocity of the initial unfragmented gas cluster ion. The change of energy with retention of velocity following collisions has been experimentally verified (as for example reported in Toyoda, N. et al., “Cluster size dependence on energy and velocity distributions of gas cluster ions after collisions with residual gas,” Nucl. Instr. & Meth. in Phys. Research B 257 (2007), pp 662-665). Fragmentation may also result in redistribution of charges in the cluster fragments. Some uncharged fragments likely result and multi-charged gas cluster ions may fragment into several charged gas cluster ions and perhaps some uncharged fragments. It is understood by the inventors that design of the focusing fields in the ionizer and the extraction region may enhance the focusing of the smaller gas cluster ions and monomer ions to increase the likelihood of collision with larger gas cluster ions in the beam extraction region and in the downstream beam, thus contributing to the dissociation and/or fragmenting of the gas cluster ions.

In an embodiment of the present invention, background gas pressure in the ionizer, acceleration region, and beamline may optionally be arranged to have a higher pressure than is normally utilized for good GCIB transmission. This can result in additional evolution of monomers from gas cluster ions (beyond that resulting from the heating and/or excitement resulting from the initial gas cluster ionization event). Pressure may be arranged so that gas cluster ions have a short enough mean-free-path and a long enough flight path between ionizer and workpiece that they must undergo multiple collisions with background gas molecules.

For a homogeneous gas cluster ion containing N monomers and having a charge state of q and which has been accelerated through an electric field potential drop of V_(Acc) volts, the cluster will have an energy of approximately qV_(Acc)/N₁ eV per monomer, where N₁ is the number of monomers in the cluster ion at the time of acceleration. Except for the smallest gas cluster ions, a collision of such an ion with a background gas monomer of the same gas as the cluster source gas will result in additional deposition of approximately qV_(Acc)/N₁ eV into the gas cluster ion. This energy is relatively small compared to the overall gas cluster ion energy (qV_(Acc)) and generally results in excitation or heating of the cluster and in subsequent evolution of monomers from the cluster. It is believed that such collisions of larger clusters with background gas seldom fragment the cluster but rather heats and/or excites it to result in evolution of monomers by evaporation or similar mechanisms. Regardless of the source of the excitation that results in the evolution of a monomer or monomers from a gas cluster ion, the evolved monomer(s) have approximately the same energy per particle, qV_(Acc)/N₁ eV, and retain approximately the same velocity and trajectory as the gas cluster ion from which they have evolved. When such monomer evolutions occur from a gas cluster ion, whether they result from excitation or heating due to the original ionization event, a collision, or radiant heating, the charge has a high probability of remaining with the larger residual gas cluster ion. Thus after a sequence of monomer evolutions, a large gas cluster ion may be reduced to a cloud of co-traveling monomers with perhaps a smaller residual gas cluster ion (or possibly several if fragmentation has also occurred). The co-traveling monomers following the original beam trajectory all have approximately the same velocity as that of the original gas cluster ion and each has energy of approximately qV_(Acc)/N₁ eV. For small gas cluster ions, the energy of collision with a background gas monomer is likely to completely and violently dissociate the small gas cluster and it is uncertain whether in such cases the resulting monomers continue to travel with the beam or are ejected from the beam.

To avoid contamination of the beam by collisions with the background gas, it is preferred that the background gas be the same gas as the gas constituting the gas cluster ions. Nozzles for forming gas cluster jets are typically operated with high gas flow on the order of 100-600 sccm. The portion of this flow that does not condense into gas clusters raises the pressure in the source chamber. In addition to the gas transmitted through the skimmer aperture in the form of gas clusters, unclustered source gas from the source chamber can flow through the skimmer aperture to the downstream beamline or beam path chamber(s). Selecting the skimmer aperture diameter to provide an increased flow of unclustered source gas from the source chamber to the beamline is a convenient way to provide the added beamline pressure to induce background gas collisions with the GCIB. Because of the high source gas flow (unclustered gas through the skimmer aperture and gas transported to the target by the beam) atmospheric gases are quickly purged from the beamline. Alternatively, gas may be leaked into the beamline chamber, or as pointed out above, introduced as a jet crossing the GCIB path. In such case, the gas is preferably the same as the source gas (or inert or otherwise non-contaminating). In critical applications a residual gas analyzer can be employed in the beamline to confirm the quality of the background gas, when background gas collisions play a role in the evolution of monomers.

Prior to the GCIB reaching the workpiece, the remaining charged particles (gas cluster ions, particularly small and intermediate size gas cluster ions and some charged monomers, but also including any remaining large gas cluster ions) in the beam are separated from the neutral portion of the beam, leaving only a Neutral Beam for processing the workpiece.

In typical operation, the fraction of power in the Neutral Beam relative to that in the full (charged plus neutral) beam delivered at the processing target is in the range of from about 5% to 95%, so by the separation methods and apparatus disclosed herein it is possible to deliver that portion of the kinetic energy of the full accelerated charged beam to the target as a Neutral Beam.

The dissociation of the gas cluster ions and thus the production of high neutral monomer beam energy is facilitated by:

1) Operating at higher acceleration voltages. This increases qV_(Acc)/N for any given cluster size; 2) Operating at high ionizer efficiency. This increases qV_(Acc)/N for any given cluster size by increasing q and increases cluster-ion on cluster-ion collisions in the extraction region due to the differences in charge states between clusters; 3) Operating at a high ionizer, acceleration region, or beamline pressure or operating with a gas jet crossing the beam, or with a longer beam path, all of which increase the probability of background gas collisions for a gas cluster ion of any given size; 4) Operating with laser irradiation or thermal radiant heating of the beam, which directly promote evolution of monomers from the gas cluster ions; and

5) Operating at higher nozzle gas flow, which increases transport of gas, clustered and perhaps unclustered into the GCIB trajectory, which increases collisions resulting in greater evolution of monomers.

For producing background gas collisions, the product of the gas cluster ion beam path length from extraction region to workpiece times the pressure in that region contributes to the degree of dissociation of the gas cluster ions that occurs. For 30 kV acceleration, ionizer parameters that provide a mean gas cluster ion charge state of 1 or greater, and a pressure times beam path length of 6×10⁻³ torr-cm (0.8 pascal-cm) (at 25 deg C) provides a Neutral Beam (after separation from the residual charged ions) that is essentially fully dissociated to neutral energetic monomers. It is convenient and customary to characterize the pressure times beam path length as a gas target thickness. 6×10⁻³ torr-cm (0.8 pascal-cm) corresponds to a gas target thickness of approximately 1.94×10¹⁴ gas molecules/cm². In one exemplary (not for limitation) embodiment the background gas pressure is 6×10⁻⁵ torr (8×10⁻³ pascal) and the beam path length is 100 cm, the acceleration potential is 30 kV, and in this case the Neutral Beam is observed to be essentially fully dissociated into monomers at the end of the beam path. This is without laser or radiant beam heating and without employing a gas jet crossing the beam. The fully dissociated accelerated Neutral Beam condition results from monomer evolution from cluster heating due to the cluster ionization event, collisions with residual gas monomers, and collisions between clusters in the beam.

Using the dissociated Neutral Beam produces improved smoothing results on smoothing a gold film compared to the full beam. In another application, using the dissociated Neutral Beam on a drug surface coating on a medical device, or on drug-polymer-mixture layer on a medical device or on a drug-poly-mixture body of a medical device provides improved drug attachment and modification of a drug elution rate without the drug weight loss that occurs when the full GCIB is used.

Measurement of the Neutral Beam cannot be made by current measurement as is convenient for gas cluster ion beams. A Neutral Beam power sensor is used to facilitate dosimetry when irradiating a workpiece with a Neutral Beam. The Neutral

Beam sensor is a thermal sensor that intercepts the beam (or optionally a known sample of the beam). The rate of rise of temperature of the sensor is related to the energy flux resulting from energetic beam irradiation of the sensor. The thermal measurements must be made over a limited range of temperatures of the sensor to avoid errors due to thermal re-radiation of the energy incident on the sensor. For a GCIB process, the beam power (watts) is equal to the beam current (amps) times V_(Acc), the beam acceleration voltage. When a GCIB irradiates a workpiece for a period of time (seconds), the energy (joules) received by the workpiece is the product of the beam power and the irradiation time. The processing effect of such a beam when it processes an extended area is distributed over the area (for example, cm²). For ion beams, it has been conveniently conventional to specify a processing dose in terms of irradiated ions/cm², where the ions are either known or assumed to have at the time of acceleration an average charge state, q, and to have been accelerated through a potential difference of , V_(Acc) volts, so that each ion carries an energy of q V_(Acc) eV (an eV is approximately 1.6×10⁻¹⁹ joule). Thus an ion beam dose for an average charge state, q, accelerated by V_(Acc) and specified in ions/cm² corresponds to a readily calculated energy dose expressible in joules/cm². For an accelerated Neutral Beam derived from an accelerated GCIB as utilized in embodiments of the present invention, the value of q at the time of acceleration and the value of V_(Acc) is the same for both of the (later- formed and separated) charged and uncharged fractions of the beam. The power in the two (neutral and charged) fractions of the GCIB divides proportional to the mass in each beam fraction. Thus for the accelerated Neutral Beam as employed in embodiments of the invention, when equal areas are irradiated for equal times, the energy dose (joules/cm²) deposited by the Neutral Beam is necessarily less than the energy dose deposited by the full GCIB. By using a thermal sensor to measure the power in the full GCIB, P_(G), and that in the Neutral Beam, P_(N), (which is commonly found to be from about 5% to about 95% that of the full GCIB) it is possible to calculate a compensation factor for use in the Neutral Beam processing dosimetry. When P_(N) is equal to aP_(G), then the compensation factor is, k=1/a. Thus if a workpiece is processed using a Neutral Beam derived from a GCIB, for a time duration is made to be k times greater than the processing duration for the full GCIB (including charged and neutral beam portions) required to achieve a dose of D ions/cm², then the energy doses deposited in the workpiece by both the Neutral Beam and the full GCIB are the same (though the results may be different due to qualitative differences in the processing effects due to differences of particle sizes in the two beams.) As used herein, a Neutral Beam process dose compensated in this way is sometimes described as having an energy/cm² equivalence of a dose of D ions/cm².

Use of a Neutral Beam derived from a gas cluster ion beam in combination with a thermal power sensor for dosimetry in many cases has advantages compared with the use of the full gas cluster ion beam or an intercepted or diverted portion, which inevitably comprises a mixture of gas cluster ions and neutral gas clusters and/or neutral monomers, and which is conventionally measured for dosimetry purposes by using a beam current measurement. Some advantages are as follows:

1) The dosimetry can be more precise with the Neutral Beam using a thermal sensor for dosimetry because the total power of the beam is measured. With a GCIB employing the traditional beam current measurement for dosimetry, only the contribution of the ionized portion of the beam is measured and employed for dosimetry. Minute-to-minute and setup-to-setup changes to operating conditions of the GCIB apparatus may result in variations in the fraction of neutral monomers and neutral clusters in the GCIB. These variations can result in process variations that may be less controlled when the dosimetry is done by beam current measurement.

2) With a Neutral Beam, a wide variety of materials may be processed, including highly insulating materials and other materials that may be damaged by electrical charging effects, without the necessity of providing a source of target neutralizing electrons to prevent workpiece charging due to charge transported to the workpiece by an ionized beam. When employed with conventional GCIB, target neutralization to reduce charging is seldom perfect, and the neutralizing electron source itself often introduces problems such as workpiece heating, contamination from evaporation or sputtering in the electron source, etc. Since a Neutral Beam does not transport charge to the workpiece, such problems are reduced.

3) There is no necessity for an additional device such as a large aperture high strength magnet to separate energetic monomer ions from the Neutral Beam. In the case of conventional GCIB the risk of energetic monomer ions (and other small cluster ions) being transported to the workpiece, where they penetrate producing deep damage, is significant and an expensive magnetic filter is routinely required to separate such particles from the beam. In the case of the Neutral Beam apparatus disclosed herein, the separation of all ions from the beam to produce the Neutral Beam inherently removes all monomer ions.

As used herein, the term “drug” is intended to mean a therapeutic agent or a material that is active in a generally beneficial way, which can be released or eluted locally in the vicinity of an implantable medical device to facilitate implanting (for example, without limitation, by providing lubrication) the device, or to facilitate (for example, without limitation, through biological or biochemical activity) a favorable medical or physiological outcome of the implantation of the device. The meaning of “drug” is intended to include a mixture of a drug with a polymer that is employed for the purpose of binding or providing coherence to the drug, attaching the drug to the medical device, or for forming a barrier layer to control release or elution of the drug. A drug that has been modified by ion beam irradiation to densify, carbonize or partially carbonize, partially denature, cross-link or partially cross-link, or to at least partially polymerize molecules of the drug is intended to be included in the “drug” definition.

As used herein, the term “intermediate size”, when referring to gas cluster size or gas cluster ion size is intended to mean sizes of from N=10 to N=1500.

As used herein, the terms “GCIB”, “gas cluster ion beam” and “gas cluster ion” are intended to encompass not only ionized beams and ions, but also accelerated beams and ions that have had all or a portion of their charge states modified (including neutralized) following their acceleration. The terms “GCIB” and “gas cluster ion beam” are intended to encompass all beams that comprise accelerated gas clusters even though they may also comprise non-clustered particles. As used herein, the term “Neutral Beam” is intended to mean a beam of neutral gas clusters and/or neutral monomers derived from an accelerated gas cluster ion beam and wherein the acceleration results from acceleration of a gas cluster ion beam.

As used herein in referencing a particle in a gas or a particle in a beam, the term “monomer” refers equally to either a single atom or a single molecule. The terms “atom,” “molecule,” and “monomer” may be used interchangeably and all refer to the appropriate monomer that is characteristic of the gas under discussion (either a component of a cluster, a component of a cluster ion, or an atom or molecule). For example, a monatomic gas like argon may be referred to in terms of atoms, molecules, or monomers and each of those terms means a single atom. Likewise, in the case of a diatomic gas like nitrogen, it may be referred to in terms of atoms, molecules, or monomers, each term meaning a diatomic molecule. Furthermore a molecular gas like CO₂ or B₂H₆, may be referred to in terms of atoms, molecules, or monomers, each term meaning a polyatomic molecule. These conventions are used to simplify generic discussions of gases and gas clusters or gas cluster ions independent of whether they are monatomic, diatomic, or molecular in their gaseous form. In referring to a constituent of a molecule or of a solid material, “atom” has its conventional meaning.

BRIEF DESCRIPTION OF THE DRAWINGS

For a better understanding of the present invention, together with other and further objects thereof, reference is made to the accompanying drawings, wherein:

FIG. 1 is a schematic illustrating elements of a prior art apparatus for processing a workpiece using a GCIB;

FIG. 2 is a schematic illustrating elements of another prior art apparatus for workpiece processing using a GCIB, wherein scanning of the ion beam and manipulation of the workpiece is employed;

FIG. 3 is a schematic of an apparatus according to an embodiment of the invention, which uses electrostatic deflection plates to separate the charged and uncharged beam components;

FIG. 4 is a schematic of an apparatus according to the an embodiment of the invention, using a thermal sensor for Neutral Beam measurement;

FIG. 5 is a schematic of an apparatus according to an embodiment of the invention which uses deflected ion beam current collected on a suppressed deflection plate as a component of a dosimetry scheme;

FIG. 6 is a schematic of an apparatus according to an embodiment of the invention which uses a sample of the deflected ion beam collected in a faraday cup as a component of a dosimetry scheme;

FIG. 7 shows a schematic of an apparatus according to an embodiment of the invention, employing mechanical scanning for irradiating an extended workpiece uniformly with a Neutral Beam;

FIG. 8 shows a schematic of an apparatus according to an embodiment of the invention with means for controlling the gas target thickness by injecting gas into the beamline chamber;

FIG. 9 shows a schematic of an apparatus according to an embodiment of the invention, which uses an electrostatic mirror to separate charged and neutral beam components;

FIG. 10 shows a schematic of an apparatus according to an embodiment of the invention wherein an accelerate-decelerate configuration is used to separate the charged beam from the neutral beam components;

FIG. 11 shows a schematic of an apparatus according to an embodiment of the invention wherein an alternate accelerate-decelerate configuration is used to separate the charged beam from the neutral beam components;

FIGS. 12A, 12B, 12C, and 12D show processing results indicating that for a metal film, processing by a neutral component of a beam produces superior smoothing of the film compared to processing with either a full GCIB or a charged component of the beam;

FIGS. 13A and 13B show comparison of a drug coating on a cobalt-chrome coupon representing a drug eluting medical device, wherein processing with a Neutral Beam produces a superior result to processing with a full GCIB;

FIG. 14 is a schematic of a Neutral Beam processing apparatus according to an embodiment of the invention wherein magnetic separation is employed;

FIGS. 15A, 15B, and 15C are TEM images illustrating the superior interfaces produced when using Neutral Beam embodiments of the invention as compared to gas cluster ion beams;

FIG. 16 is a graph showing a SIMS profile of a shallow boron implantation suitable for forming shallow junctions, using an embodiment of the invention;

FIG. 17 is a TEM image showing a high quality interface formed when an embodiment of the invention is used in forming a boron doped semiconductor;

FIG. 18 is a graph illustrating the etching of SiO₂ and Si using an embodiment of the invention;

FIGS. 19A and 19B are TEM images illustrating the use of embodiments of the invention in forming amorphous layers in semiconductor materials;

FIGS. 20A and 20B are TEM images illustrating the application of accelerated Neutral Beams derived from GCIBs for forming films in semiconductors;

FIG. 21 is a graph illustrating the deposition of a diamond-like carbon film on a silicon substrate using an accelerated Neutral Beam derived from an accelerated GCIB;

FIG. 22 is an atomic force micrograph map of roughness of a clean, conventionally polished optical glass surface, showing a degree of roughness, lack of planarity, and the presence of asperities;

FIG. 23 is an atomic force micrograph map of an optical glass surface after smoothing according to an embodiment of the invention using an accelerated Neutral Beam derived from an accelerated GCIB;

FIGS. 24A, 24B, 24C, and 24D are schematics that show steps in a process for using an accelerated Neutral Beam derived from a GCIB or for using a GCIB for producing an optical coating on an optical substrate with superior adhesion of the coating to the substrate according to an embodiment of the invention as compared with conventional techniques;

FIGS. 25A and 25B are atomic force micrograph maps of surfaces of an untreated LBO optical component showing degradation due to atmospheric exposure;

FIGS. 26A and 26B are atomic force micrograph maps of surfaces of an LBO optical component treated using an accelerated Neutral Beam derived from a GCIB, with resulting reduced degradation due to atmospheric exposure following treatment according to an embodiment of the invention; and

FIGS. 27A, 27B, 27C, and 27D are schematics that show steps in a process for using an accelerated Neutral Beam derived from a GCIB to form a SiC or SiC_(x) layer on a silicon substrate.

DETAILED DESCRIPTION OF THE DRAWINGS

Reference is now made to FIG. 1, which shows a schematic configuration for a prior art GCIB processing apparatus 100. A low-pressure vessel 102 has three fluidly connected chambers: a nozzle chamber 104, an ionization/acceleration chamber 106, and a processing chamber 108. The three chambers are evacuated by vacuum pumps 146 a, 146 b, and 146 c, respectively. A pressurized condensable source gas 112 (for example argon) stored in a gas storage cylinder 111 flows through a gas metering valve 113 and a feed tube 114 into a stagnation chamber 116. Pressure (typically a few atmospheres) in the stagnation chamber 116 results in ejection of gas into the substantially lower pressure vacuum through a nozzle 110, resulting in formation of a supersonic gas jet 118. Cooling, resulting from the expansion in the jet, causes a portion of the gas jet 118 to condense into clusters, each consisting of from several to several thousand weakly bound atoms or molecules. A gas skimmer aperture 120 is employed to control flow of gas into the downstream chambers by partially separating gas molecules that have not condensed into a cluster jet from the cluster jet. Excessive pressure in the downstream chambers can be detrimental by interfering with the transport of gas cluster ions and by interfering with management of the high voltages that may be employed for beam formation and transport. Suitable condensable source gases 112 include, but are not limited to argon and other condensable noble gases, nitrogen, carbon dioxide, oxygen, and many other gases and/or gas mixtures. After formation of the gas clusters in the supersonic gas jet 118, at least a portion of the gas clusters are ionized in an ionizer 122 that is typically an electron impact ionizer that produces electrons by thermal emission from one or more incandescent filaments 124 (or from other suitable electron sources) and accelerates and directs the electrons, enabling them to collide with gas clusters in the gas jet 118. Electron impacts with gas clusters eject electrons from some portion of the gas clusters, causing those clusters to become positively ionized. Some clusters may have more than one electron ejected and may become multiply ionized. Control of the number of electrons and their energies after acceleration typically influences the number of ionizations that may occur and the ratio between multiple and single ionizations of the gas clusters. A suppressor electrode 142, and grounded electrode 144 extract the cluster ions from the ionizer exit aperture 126, accelerate them to a desired energy (typically with acceleration potentials of from several hundred V to several tens of kV), and focuses them to form a GCIB 128. The region that the GCIB 128 traverses between the ionizer exit aperture 126 and the suppressor electrode 142 is referred to as the extraction region. The axis (determined at the nozzle 110), of the supersonic gas jet 118 containing gas clusters is substantially the same as the axis 154 of the GCIB 128.

Filament power supply 136 provides filament voltage V_(f) to heat the ionizer filament 124. Anode power supply 134 provides anode voltage V_(A) to accelerate thermoelectrons emitted from filament 124 to cause the thermoelectrons to irradiate the cluster-containing gas jet 118 to produce cluster ions. A suppression power supply 138 supplies suppression voltage V_(s) (on the order of several hundred to a few thousand volts) to bias suppressor electrode 142. Accelerator power supply 140 supplies acceleration voltage V_(Acc) to bias the ionizer 122 with respect to suppressor electrode 142 and grounded electrode 144 so as to result in a total GCIB acceleration potential equal to V_(Acc). Suppressor electrode 142 serves to extract ions from the ionizer exit aperture 126 of ionizer 122 and to prevent undesired electrons from entering the ionizer 122 from downstream, and to form a focused GCIB 128.

A workpiece 160, which may (for example) be a medical device, a semiconductor material, an optical element, or other workpiece to be processed by GCIB processing, is held on a workpiece holder 162, that disposes the workpiece in the path of the GCIB 128. The workpiece holder is attached to but electrically insulated from the processing chamber 108 by an electrical insulator 164. Thus, GCIB 128 striking the workpiece 160 and the workpiece holder 162 flows through an electrical lead 168 to a dose processor 170. A beam gate 172 controls transmission of the GCIB 128 along axis 154 to the workpiece 160. The beam gate 172 typically has an open state and a closed state that is controlled by a linkage 174 that may be (for example) electrical, mechanical, or electromechanical. Dose processor 170 controls the open/closed state of the beam gate 172 to manage the GCIB dose received by the workpiece 160 and the workpiece holder 162. In operation, the dose processor 170 opens the beam gate 172 to initiate GCIB irradiation of the workpiece 160. Dose processor 170 typically integrates GCIB electrical current arriving at the workpiece 160 and workpiece holder 162 to calculate an accumulated GCIB irradiation dose. At a predetermined dose, the dose processor 170 closes the beam gate 172, terminating processing when the predetermined dose has been achieved.

In the following description, for simplification of the drawings, item numbers from earlier figures may appear in subsequent figures without discussion. Likewise, items discussed in relation to earlier figures may appear in subsequent figures without item numbers or additional description. In such cases items with like numbers are like items and have the previously described features and functions and illustration of items without item numbers shown in the present figure refer to like items having the same functions as the like items illustrated in earlier numbered figures.

FIG. 2 shows a schematic illustrating elements of another prior art GCIB processing apparatus 200 for workpiece processing using a GCIB, wherein scanning of the ion beam and manipulation of the workpiece is employed. A workpiece 160 to be processed by the GCIB processing apparatus 200 is held on a workpiece holder 202, disposed in the path of the GCIB 128. In order to accomplish uniform processing of the workpiece 160, the workpiece holder 202 is designed to manipulate workpiece 160, as may be required for uniform processing.

Any workpiece surfaces that are non-planar, for example, spherical or cup-like, rounded, irregular, or other un-flat configuration, may be oriented within a range of angles with respect to the beam incidence to obtain optimal GCIB processing of the workpiece surfaces. The workpiece holder 202 can be fully articulated for orienting all non-planar surfaces to be processed in suitable alignment with the GCIB 128 to provide processing optimization and uniformity. More specifically, when the workpiece 160 being processed is non-planar, the workpiece holder 202 may be rotated in a rotary motion 210 and articulated in articulation motion 212 by an articulation/rotation mechanism 204. The articulation/rotation mechanism 204 may permit 360 degrees of device rotation about longitudinal axis 206 (which is coaxial with the axis 154 of the GCIB 128) and sufficient articulation about an axis 208 perpendicular to axis 206 to maintain the workpiece surface to within a desired range of beam incidence.

Under certain conditions, depending upon the size of the workpiece 160, a scanning system may be desirable to produce uniform irradiation of a large workpiece. Although often not necessary for GCIB processing, two pairs of orthogonally oriented electrostatic scan plates 130 and 132 may be utilized to produce a raster or other scanning pattern over an extended processing area. When such beam scanning is performed, a scan generator 156 provides X-axis scanning signal voltages to the pair of scan plates 132 through lead pair 159 and Y-axis scanning signal voltages to the pair of scan plates 130 through lead pair 158. The scanning signal voltages are commonly triangular waves of different frequencies that cause the GCIB 128 to be converted into a scanned GCIB 148, which scans the entire surface of the workpiece 160. A scanned beam-defining aperture 214 defines a scanned area. The scanned beam-defining aperture 214 is electrically conductive and is electrically connected to the low-pressure vessel 102 wall and supported by support member 220. The workpiece holder 202 is electrically connected via a flexible electrical lead 222 to a faraday cup 216 that surrounds the workpiece 160 and the workpiece holder 202 and collects all the current passing through the defining aperture 214. The workpiece holder 202 is electrically isolated from the articulation/rotation mechanism 204 and the faraday cup 216 is electrically isolated from and mounted to the low-pressure vessel 102 by insulators 218. Accordingly, all current from the scanned GCIB 148, which passes through the scanned beam-defining aperture 214 is collected in the faraday cup 216 and flows through electrical lead 224 to the dose processor 170. In operation, the dose processor 170 opens the beam gate 172 to initiate GCIB irradiation of the workpiece 160. The dose processor 170 typically integrates GCIB electrical current arriving at the workpiece 160 and workpiece holder 202 and faraday cup 216 to calculate an accumulated GCIB irradiation dose per unit area. At a predetermined dose, the dose processor 170 closes the beam gate 172, terminating processing when the predetermined dose has been achieved. During the accumulation of the predetermined dose, the workpiece 160 may be manipulated by the articulation/rotation mechanism 204 to ensure processing of all desired surfaces.

FIG. 3 is a schematic of a Neutral Beam processing apparatus 300 according to an embodiment of the invention, which uses electrostatic deflection plates to separate the charged and uncharged portions of a GCIB. A beamline chamber 107 encloses the ionizer and accelerator regions and the workpiece processing regions. The beamline chamber 107 has high conductance and so the pressure is substantially uniform throughout. A vacuum pump 146 b evacuates the beamline chamber 107. Gas flows into the beamline chamber 107 in the form of clustered and unclustered gas transported by the gas jet 118 and in the form of additional unclustered gas that leaks through the gas skimmer aperture 120. A pressure sensor 330 transmits pressure data from the beamline chamber 107 through an electrical cable 332 to a pressure sensor controller 334, which measures and displays pressure in the beamline chamber 107. The pressure in the beamline chamber 107 depends on the balance of gas flow into the beamline chamber 107 and the pumping speed of the vacuum pump 146 b. By selection of the diameter of the gas skimmer aperture 120, the flow of source gas 112 through the nozzle 110, and the pumping speed of the vacuum pump 146 b, the pressure in the beamline chamber 107 equilibrates at a pressure, PB, determined by design and by nozzle flow. The GCIB flight path from grounded electrode 144 to workpiece holder 162, is for example, 100 cm. By design and adjustment PB may be approximately 6×10⁻⁵ torr (8×10⁻³ pascal). Thus the product of pressure and beam path length is approximately 6×10⁻³ torr-cm (0.8 pascal-cm) and the gas target thickness for the beam is approximately 1.94×10¹⁴ gas molecules per cm², which combined with monomer evolution due to the initial ionization of the gas clusters in the ionizer 122 and collisions that occur between gas cluster ions in the GCIB 128 is observed to be effective for dissociating the gas cluster ions in the GCIB 128 and results in a fully dissociated accelerated Neutral Beam 314. V_(Acc) may be for example 30kV and the GCIB 128 is accelerated by that potential. A pair of deflection plates (302 and 304) is disposed about the axis 154 of the GCIB 128. A deflector power supply 306 provides a positive deflection voltage V_(D) to deflection plate 302 via electrical lead 308. Deflection plate 304 is connected to electrical ground by electrical lead 312 and through current sensor/display 310. Deflector power supply 306 is manually controllable. V_(D) may be adjusted from zero to a voltage sufficient to completely deflect the ionized portion 316 of the GCIB 128 onto the deflection plate 304 (for example a few thousand volts). When the ionized portion 316 of the GCIB 128 is deflected onto the deflection plate 304, the resulting current, I_(D) flows through electrical lead 312 and current sensor/display 310 for indication. When V_(D) is zero, the GCIB 128 is undeflected and travels to the workpiece 160 and the workpiece holder 162. The GCIB beam current I_(B) is collected on the workpiece 160 and the workpiece holder 162 and flows through electrical lead 168 and current sensor/display 320 to electrical ground. I_(B) is indicated on the current sensor/display 320. A beam gate 172 is controlled through a linkage 338 by beam gate controller 336. Beam gate controller 336 may be manual or may be electrically or mechanically timed by a preset value to open the beam gate 172 for a predetermined interval. In use, V_(D) is set to zero, and the beam current, I_(B), striking the workpiece holder is measured. Based on previous experience for a given GCIB process recipe, an initial irradiation time for a given process is determined based on the measured current, I_(B). V_(D) is increased until all measured beam current is transferred from I_(B) to I_(D) and I_(D) no longer increases with increasing V_(D). At this point a Neutral Beam 314 comprising energetic dissociated components of the initial GCIB 128 irradiates the workpiece holder 162. The beam gate 172 is then closed and the workpiece 160 placed onto the workpiece holder 162 by conventional workpiece loading means (not shown). The beam gate 172 is opened for the predetermined initial radiation time. After the irradiation interval, the workpiece may be examined and the processing time adjusted as necessary to calibrate the desired duration of Neutral Beam processing based on the measured GCIB beam current I_(B). Following such a calibration process, additional workpieces may be processed using the calibrated exposure duration.

The Neutral Beam 314 contains a repeatable fraction of the initial energy of the accelerated GCIB 128. The remaining ionized portion 316 of the original GCIB 128 has been removed from the Neutral Beam 314 and is collected by the grounded deflection plate 304. The ionized portion 316 that is removed from the Neutral Beam 314 may include monomer ions and gas cluster ions including intermediate size gas cluster ions. Because of the monomer evaporation mechanisms due to cluster heating during the ionization process, intra-beam collisions, background gas collisions, and other causes (all of which result in erosion of clusters) the Neutral Beam substantially consists of neutral monomers, while the separated charged particles are predominately cluster ions. The inventors have confirmed this by suitable measurements that include re-ionizing the Neutral Beam and measuring the charge to mass ratio of the resulting ions. The separated charged beam components largely consist of cluster ions of intermediate size as well as monomer ions and perhaps some large cluster ions. As will be shown below, certain superior process results are obtained by processing workpieces using this Neutral Beam.

FIG. 4 is a schematic of a Neutral Beam processing apparatus 400 according to an embodiment of the invention, which uses a thermal sensor for Neutral Beam measurement. A thermal sensor 402 attaches via low thermal conductivity attachment 404 to a rotating support arm 410 attached to a pivot 412. Actuator 408 moves thermal sensor 402 via a reversible rotary motion 416 between positions that intercept the Neutral Beam 314 or GCIB 128 and a parked position indicated by 414 where the thermal sensor 402 does not intercept any beam. When thermal sensor 402 is in the parked position (indicated by 414) the GCIB 128 or Neutral Beam 314 continues along path 406 for irradiation of the workpiece 160 and/or workpiece holder 162. A thermal sensor controller 420 controls positioning of the thermal sensor 402 and performs processing of the signal generated by thermal sensor 402. Thermal sensor 402 communicates with the thermal sensor controller 420 through an electrical cable 418. Thermal sensor controller 420 communicates with a dosimetry controller 432 through an electrical cable 428. A beam current measurement device 424 measures beam current I_(B) flowing in electrical lead 168 when the GCIB 128 strikes the workpiece 160 and/or the workpiece holder 162. Beam current measurement device 424 communicates a beam current measurement signal to dosimetry controller 432 via electrical cable 426. Dosimetry controller 432 controls setting of open and closed states for beam gate 172 by control signals transmitted via linkage 434. Dosimetry controller 432 controls deflector power supply 440 via electrical cable 442 and can control the deflection voltage V_(D) between voltages of zero and a positive voltage adequate to completely deflect the ionized portion 316 of the GCIB 128 to the deflection plate 304. When the ionized portion 316 of the GCIB 128 strikes deflection plate 304, the resulting current I_(D) is measured by current sensor 422 and communicated to the dosimetry controller 432 via electrical cable 430. In operation dosimetry controller 432 sets the thermal sensor 402 to the parked position 414, opens beam gate 172, sets V_(D) to zero so that the full GCIB 128 strikes the workpiece holder 162 and/or workpiece 160. The dosimetry controller 432 records the beam current I_(B) transmitted from beam current measurement device 424. The dosimetry controller 432 then moves the thermal sensor 402 from the parked position 414 to intercept the GCIB 128 by commands relayed through thermal sensor controller 420. Thermal sensor controller 420 measures the beam energy flux of GCIB 128 by calculation based on the heat capacity of the sensor and measured rate of temperature rise of the thermal sensor 402 as its temperature rises through a predetermined measurement temperature (for example 70 degrees C.) and communicates the calculated beam energy flux to the dosimetry controller 432 which then calculates a calibration of the beam energy flux as measured by the thermal sensor 402 and the corresponding beam current measured by the beam current measurement device 424. The dosimetry controller 432 then parks the thermal sensor 402 at parked position 414, allowing it to cool and commands application of positive V_(D) to deflection plate 302 until all of the current I_(D) due to the ionized portion of the GCIB 128 is transferred to the deflection plate 304. The current sensor 422 measures the corresponding I_(D) and communicates it to the dosimetry controller 432. The dosimetry controller also moves the thermal sensor 402 from parked position 414 to intercept the Neutral Beam 314 by commands relayed through thermal sensor controller 420. Thermal sensor controller 420 measures the beam energy flux of the Neutral Beam 314 using the previously determined calibration factor and the rate of temperature rise of the thermal sensor 402 as its temperature rises through the predetermined measurement temperature and communicates the Neutral Beam energy flux to the dosimetry controller 432. The dosimetry controller 432 calculates a neutral beam fraction, which is the ratio of the thermal measurement of the Neutral Beam 314 energy flux to the thermal measurement of the full GCIB 128 energy flux at sensor 402. Under typical operation, a neutral beam fraction of about 5% to about 95% is achieved. Before beginning processing, the dosimetry controller 432 also measures the current, I_(D), and determines a current ratio between the initial values of I_(B) and I_(D). During processing, the instantaneous I_(D) measurement multiplied by the initial I_(B)/I_(D) ratio may be used as a proxy for continuous measurement of the I_(B) and employed for dosimetry during control of processing by the dosimetry controller 432. Thus the dosimetry controller 432 can compensate any beam fluctuation during workpiece processing, just as if an actual beam current measurement for the full GCIB 128 were available. The dosimetry controller uses the neutral beam fraction to compute a desired processing time for a particular beam process. During the process, the processing time can be adjusted based on the calibrated measurement of I_(D) for correction of any beam fluctuation during the process.

FIG. 5 is a schematic of a Neutral Beam processing apparatus 500 according to an embodiment of the invention that uses deflected ion beam current collected on a suppressed deflection plate as a component of a dosimetry scheme. Referring briefly to FIG. 4, the dosimetry scheme shown in FIG. 4 can suffer from the fact that the current, ID, includes the current due to the ionized portion 316 of the GCIB 128 as well as secondary electron currents resulting from ejection of secondary electrons emitted when the ionized portion 316 of the beam strikes deflection plate 304. The secondary electron yield can vary depending on the distribution of cluster ion sizes in the ionized portion 316. It can also vary depending on the surface state (cleanliness, etc.) of the impacted surface of the deflection plate 304. Thus, in the scheme described in FIG. 4, the magnitude of I_(D) is not a precise representation of the current due to the ionized portion 316 of the GCIB 128. Referring again now to FIG. 5, an improved measurement of the ionized portion 316 of GCIB 128 can be realized at deflection plate 304 by adding an electron suppressor grid electrode 502 proximal to the surface of deflection plate 304 that receives the ionized portion 316. The electron suppressor grid electrode 502 is highly transparent to the ionized portion 316, but is biased negative with respect to the deflection plate 304 by second suppressor voltage V_(S2) provided by second suppressor power supply 506. Effective suppression of secondary electrons is typically achieved by a V_(S2) on the order of several tens of volts. By suppressing the emission of secondary electrons, the current loading of deflector power supply 440 is reduced and the precision of the I_(D) representation of the current in the ionized portion 316 of the GCIB 128 is increased. Electron suppressor grid 502 is insulated from and maintained in proximity to deflection plate 304 by insulating supports 504.

FIG. 6 is a schematic of a Neutral Beam processing apparatus 550 according to an embodiment of the invention that uses a sample of deflected ion beam current collected in a faraday cup as a component of a dosimetry scheme. In this embodiment of the invention, a sample 556 of the ionized portion 316 (as shown in FIG. 5) is captured in a faraday cup 558. Sample current, I_(S), collected in the faraday cup 558 is conducted via electrical lead 560 to current sensor 562 for measurement, and the measurement is communicated to a dosimetry controller 566 via electrical cable 564. Faraday cup 558 provides a superior current measurement to that obtained by measuring the current I_(D) collected by deflection plate 304 (as shown in FIG. 5). Current sensor 562 operates substantially as previously described for the current sensor 422 (as shown in FIG. 5) except that current sensor 562 has increased sensitivity to accommodate the smaller magnitude of I_(S) as compared to I_(D). Dosimetry controller 566 operates substantially as previously described for dosimetry controller 432 (as shown in FIG. 5) except that it is designed to accommodate a smaller current measurement I_(S) (as compared to I_(D) of FIG. 5).

FIG. 7 is a schematic of a Neutral Beam processing apparatus 600 according to an embodiment of the invention that uses mechanical scanner 602 to scan a spatially extended workpiece 160 through the Neutral Beam 314 to facilitate uniform Neutral Beam scanning of a large workpiece. Since the Neutral Beam 314 cannot be scanned by magnetic or electrostatic techniques, when the workpiece 160 to be processed is spatially larger than the extent of the Neutral Beam 314 and uniform processing of the workpiece 160 is required, a mechanical scanner 602 is employed to scan the workpiece 160 through the Neutral Beam 314. Mechanical scanner 602 has a workpiece holder 616 for holding workpiece 160. The mechanical scanner 602 is disposed so that either the Neutral Beam 314 or the GCIB 128 can be incident on the workpiece 160 and/or the workpiece holder 616. When the deflection plates (302, 304) deflect the ionized portion 316 out of the GCIB 128, the workpiece 160 and/or the workpiece holder 616 receive only the Neutral Beam 314. When the deflection plates (302, 304) do not deflect the ionized portion 316 of the GCIB 128, the workpiece 160 and/or the workpiece holder 616 receives the full GCIB 128. Workpiece holder 616 is electrically conductive and is insulated from ground by insulator 614. Beam current (I_(B)) due to GCIB 128 incident on the workpiece 160 and/or the workpiece holder 616 is conducted to beam current measurement device 424 via electrical lead 168. Beam current measurement device 424 measures I_(B) and communicates the measurement to dosimetry controller 628. Mechanical scanner 602 has an actuator base 604 containing actuators controlled by mechanical scan controller 618 via electrical cable 620. Mechanical scanner 602 has a Y-displacement table 606 capable of reversible motion in an Y-direction 610, and it has an X-displacement table 608 capable of reversible motion in an X-direction 612, indicated as in and out of the plane of the paper of FIG. 7. Movements of the Y-displacement table 606 and of the X-displacement table 608 are actuated by actuators in the actuator base 604 under control of the mechanical scan controller 618. Mechanical scan controller 618 communicates via electrical cable 622 with dosimetry controller 628. Function of dosimetry controller 628 includes all functions previously described for dosimetry controller 432, with additional function for controlling the mechanical scanner 602 via communication with mechanical scan controller 618. Based on measured Neutral Beam energy flux rate, dosimetry controller 628 calculates and communicates to mechanical scan controller 618 the Y- and X-scanning rates for causing an integral number of complete scans of the workpiece 160 to be completed during processing of a workpiece 160, insuring complete and uniform processing of the workpiece and insures a predetermined energy flux dose to the workpiece 160. Except for the use of a Neutral Beam, and the use of a Neutral Beam energy flux rate measurement, such scanning control algorithms are conventional and commonly employed in, for examples, conventional GCIB processing tools and in ion implantation tools. It is noted that the Neutral Beam processing apparatus 600 can be used as a conventional GCIB processing tool by controlling the deflection plates (302, 304) so that GCIB 128 passes without deflection, allowing the full GCIB 128 to irradiate the workpiece 160 and/or the workpiece holder 616.

FIG. 8 is a schematic of a Neutral Beam processing apparatus 700 according to an embodiment of the invention that provides active setting and control of the gas pressure in the beamline chamber 107. A pressure sensor 330 transmits pressure measurement data from the beamline chamber 107 through an electrical cable 332 to a pressure controller 716, which measures and displays pressure in the beamline chamber. The pressure in the beamline chamber 107 depends on the balance of gas flow into the beamline chamber 107 and the pumping speed of the vacuum pump 146 b. A gas bottle 702 contains a beamline gas 704 that is preferably the same gas species as the source gas 112. Gas bottle 702 has a remotely operable leak valve 706 and a gas feed tube 708 for leaking beamline gas 704 into the beamline chamber 107 through a gas diffuser 710 in the beamline chamber 107. The pressure controller 716 is capable of receiving an input set point (by manual entry or by automatic entry from an system controller (not shown)) in the form of a pressure set point, a pressure times beam path length set point (based on predetermined beam path length), or a gas target thickness set point. Once a set point has been established for the pressure controller 716, it regulates the flow of beamline gas 704 into the beamline chamber 107 to maintain the set point during operation of the Neutral Beam processing apparatus. When such a beamline pressure regulation system is employed, the vacuum pump 146 b is normally sized so that in the absence of beamline gas 704 being introduced into the beamline chamber 107, the baseline pressure in the beamline chamber 107 is lower than the desired operating pressure. If the baseline pressure is chosen so that the conventional GCIB 128 can propagate the length of the beam path without excessive dissociation, then the Neutral Beam processing apparatus 700 can also be used as a conventional GCIB processing tool.

FIG. 9 is a schematic of a Neutral Beam processing apparatus 800 according to an embodiment of the invention that employs an electrostatic mirror for separation of the charged and neutral beam portions. A reflecting electrode 802 and a substantially transparent electrical grid electrode 804 are disposed displaced from each other, parallel to each other, and at a 45-degree angle to the beam axis 154. The reflecting electrode 802 and the substantially transparent electrical grid electrode 804 both have holes (836 and 838 respectively) centered on the beam axis 154 for permitting passage of the Neutral Beam 314 through the two electrodes. A mirror power supply 810 provides a mirror electrical potential V_(M) across the gap between the reflecting electrode 802 and the substantially transparent electrical grid electrode 804 via electrical leads 806 and 808, with polarity as indicated in FIG. 9. VM is selected to be slightly greater than V_(Acc)+V_(R) (V_(R) being the retarding potential required to overcome the thermal energy the gas cluster jet has before ionization and acceleration—V_(R) is typically on the order of a few kV). The electric field generated between the reflecting electrode 802 and the substantially transparent electrical grid electrode 804 deflects the ionized portion 814 of the GCIB 128 through approximately a 90-degree angle with respect to the axis 154. A faraday cup 812 is disposed to collect the ionized portion 814 of the GCIB 128. A suppressor electrode grid electrode 816 prevents escape of secondary electrons from the faraday cup 812. The suppressor grid electrode 816 is biased with a negative third suppressor voltage V_(S3) provided by third suppressor power supply 822. V_(S3) is typically on the order of several tens of volts. The faraday cup current, I_(D2), representing current in the deflected ionized portion 814 of the GCIB 128 (and thus the current in the GCIB 128) flows through electrical lead 820 to current sensor 824. Current sensor 824 measures the current I_(D2) and transmits the measurement to dosimetry controller 830 via electrical lead 826. The function of dosimetry controller 830 is as previously described for dosimetry controller 432, except that dosimetry controller 830 receives I_(D2) current measurement information from current sensor 824 and dosimetry controller 830 does not control deflector power supply 440, but instead controls mirror power supply 810 via electrical cable 840. By setting mirror power supply 810 to output either zero volts or V_(M), dosimetry controller 830 controls whether the full GCIB 128, or only the Neutral Beam 314 of GCIB 128 is transmitted to the workpiece 160 and/or workpiece holder 616 for measurement and/or processing.

FIG. 10 is a schematic of a Neutral Beam processing apparatus 940 according to an embodiment of the invention, which has the advantage of both the ionizer 122 and the workpiece 160 operating at ground potential. The workpiece 160 is held in the path of Neutral Beam 314 by electrically conductive workpiece holder 162, which in turn is supported by electrically conductive support member 954 attached to a wall of the low-pressure vessel 102. Accordingly, workpiece holder 162 and the workpiece 160 are electrically grounded. An acceleration electrode 948 extracts gas cluster ions from ionizer exit aperture 126 and accelerates the gas cluster ions through a voltage potential V_(Acc) provided by acceleration power supply 944 to form a GCIB 128. The body of ionizer 122 is grounded and V_(Acc) is of negative polarity. Neutral gas atoms in the gas jet 118 have a small energy on the order of several tens of milli-electron-volts. As they condense into clusters, this energy accumulates proportional to cluster size, N. Sufficiently large clusters gain non-negligible energies from the condensation process and when accelerated through a voltage potential of V_(Acc), the final energy of each ion exceeds V_(Acc) by its neutral cluster jet energy. Downstream of the acceleration electrode 948, a retarding electrode 952 is employed to ensure deceleration of the ionized portion 958 of the GCIB 128. Retarding electrode 952 is biased at a positive retarding voltage, VR, by retarding voltage power supply 942. A retarding voltage V_(R) of a few kV is generally adequate to ensure that all ions in the GCIB 128 are decelerated and returned to the acceleration electrode 948. Permanent magnet arrays 950 are attached to the acceleration electrode 948 to provide magnetic suppression of secondary electrons that would otherwise be emitted as a result of the returned ions striking the acceleration electrode 948. A beam gate 172 is a mechanical beam gate and is located upstream of the workpiece 160. A dosimetry controller 946 controls the process dose received by the workpiece. A thermal sensor 402 is placed into a position that intercepts the Neutral Beam 314 for Neutral Beam energy flux measurement or in the parked position for Neutral Beam processing of the workpiece under control of the thermal sensor controller 420. When thermal sensor 402 is in the beam sensing position, the Neutral Beam energy flux is measured and transmitted to the dosimetry controller 946 over electrical cable 956. In normal use, the dosimetry controller 946 closes the beam gate 172 and commands the thermal sensor controller 420 to measure and report the energy flux of the Neutral Beam 314. Next, a conventional workpiece loading mechanism (not shown) places a new workpiece on the workpiece holder. Based on the measured Neutral Beam energy flux, the dosimetry controller 946 calculates an irradiation time for providing a predetermined desired Neutral Beam energy dose. The dosimetry controller 946 commands the thermal sensor 402 out of the Neutral Beam 314 and opens the beam gate 172 for the calculated irradiation time and then closes the beam gate 172 at the end of the calculated irradiation time to terminate the processing of the workpiece 160.

FIG. 11 is a schematic of a Neutral Beam processing apparatus 960 according to an embodiment of the invention, wherein the ionizer 122 operates at a negative potential V_(R) and wherein the workpiece operates at ground potential. An acceleration electrode 948 extracts gas cluster ions from ionizer exit aperture 126 and accelerates the gas cluster ions toward a potential of V_(Acc) provided by acceleration power supply 944 to form a GCIB 128. The resulting GCIB 128 is accelerated by a potential V_(Acc)−V_(R). A ground electrode 962 decelerates the ionized portion 958 of the GCIB 128 and returns it to the acceleration electrode 948.

FIG. 14 is a schematic of a Neutral Beam processing apparatus 980 according to an embodiment of the invention. This embodiment is similar to that shown in FIG. 8, except that the separation of the charged beam components from the neutral beam components is done by means of a magnetic field, rather than an electrostatic field. Referring again to FIG. 14, a magnetic analyzer 982 has magnetic pole faces separated by a gap in which a magnetic B-field is present. Support 984 disposes the magnetic analyzer 982 relative to the GCIB 128 such that the GCIB 128 enters the gap of the magnetic analyzer 982 such that the vector of the B-field is transverse to the axis 154 of the GCIB 128. The ionized portion 990 of the GCIB 128 is deflected by the magnetic analyzer 982. A baffle 986 with a Neutral Beam aperture 988 is disposed with respect to the axis 154 so that the Neutral Beam 314 can pass through the Neutral Beam aperture 988 to the workpiece 160. The ionized portion 990 of the GCIB 128 strikes the baffle 986 and/or the walls of the low-pressure vessel 102 where it dissociates to gas that is pumped away by the vacuum pump 146 b.

FIGS. 12A through 12D show the comparative effects of full and charge separated beams on a gold thin film. In an experimental setup, a gold film deposited on a silicon substrate was processed by a full GCIB (charged and neutral components), a Neutral Beam (charged components deflected out of the beam), and a deflected beam comprising only charged components. All three conditions are derived from the same initial GCIB, a 30 kV accelerated Ar GCIB. Gas target thickness for the beam path after acceleration was approximately 2×10¹⁴ argon gas atoms per cm². For each of the three beams, exposures were matched to the total energy carried by the full beam (charged plus neutral) at an ion dose of 2×10¹⁵ gas cluster ions per cm². Energy flux rates of each beam were measured using a thermal sensor and process durations were adjusted to ensure that each sample received the same total thermal energy dose equivalent to that of the full (charged plus neutral) GCIB dose.

FIG. 12A shows an atomic force microscope (AFM) 5 micron by 5 micron scan and statistical analysis of an as-deposited gold film sample that had an average roughness, Ra, of approximately 2.22 nm. FIG. 12B shows an AFM scan of the gold surface processed with the full GCIB—average roughness, Ra, has been reduced to approximately 1.76 nm. FIG. 12C shows an AFM scan of the surface processed using only charged components of the beam (after deflection from the neutral beam components)—average roughness, Ra, has been increased to approximately 3.51 nm. FIG. 12D shows an AFM scan of the surface processed using only the neutral component of the beam (after charged components were deflected out of the Neutral Beam)—average roughness, Ra, is smoothed to approximately 1.56 nm. The full GCIB processed sample (B) is smoother than the as deposited film (A). The Neutral Beam processed sample (D) is smoother than the full GCIB processed sample (B). The sample (C) processed with the charged component of the beam is substantially rougher than the as-deposited film. The results support the conclusion that the neutral portions of the beam contribute to smoothing and the charged components of the beam contribute to roughening.

FIGS. 13A and 13B show comparative results of full GCIB and Neutral Beam processing of a drug film deposited on a cobalt-chrome coupon used to evaluate drug elution rate for a drug eluting coronary stent. FIG. 13A represents a sample irradiated using an argon GCIB (including the charged and neutral components) accelerated using V_(Acc) of 30 kV with an irradiated dose of 2×10¹⁵ gas cluster ions per cm². FIG. 13B represents a sample irradiated using a Neutral Beam derived from an argon GCIB accelerated using V_(Acc) of 30 kV. The Neutral Beam was irradiated with a thermal energy dose equivalent to that of a 30 kV accelerated , 2×10¹⁵ gas cluster ion per cm² dose (equivalent determined by beam thermal energy flux sensor). The irradiation for both samples was performed through a cobalt chrome proximity mask having an array of circular apertures of approximately 50 microns diameter for allowing beam transmission. FIG. 13A is a scanning electron micrograph of a 300 micron by 300 micron region of the sample that was irradiated through the mask with full beam. FIG. 13B is a scanning electron micrograph of a 300 micron by 300 micron region of the sample that was irradiated through the mask with a Neutral Beam. The sample shown in FIG. 13A exhibits damage and etching caused by the full beam where it passed through the mask. The sample shown in FIG. 13B exhibits no visible effect. In elution rate tests in physiological saline solution, the samples processed like the Figure B sample (but without mask) exhibited superior (delayed) elution rate compared to the samples processed like the FIG. 13A sample (but without mask). The results support the conclusion that processing with the Neutral Beam contributes to the desired delayed elution effect, while processing with the full GCIB (charged plus neutral components) contributes to weight loss of the drug by etching, with inferior (less delayed) elution rate effect.

To further illustrate the ability of an accelerated Neutral Beam derived from an accelerated GCIB to aid in attachment of a drug to a surface and to provide drug modification in such a way that it results in delayed drug elution, an additional test was performed. Silicon coupons approximately 1 cm by 1 cm (1 cm2) were prepared from highly polished clean semiconductor-quality silicon wafers for use as drug deposition substrates. A solution of the drug Rapamycin (Catalog number R-5000, LC Laboratories, Woburn, Mass. 01801, USA) was formed by dissolving 500 mg of Rapamycin in 20 ml of acetone. A pipette was then used to dispense approximately 5 micro-liter droplets of the drug solution onto each coupon. Following atmospheric evaporation and vacuum drying of the solution, this left approximately 5 mm diameter circular Rapamycin deposits on each of the silicon coupons. Coupons were divided into groups and either left un-irradiated (controls) or irradiated with various conditions of Neutral Beam irradiation. The groups were then placed in individual baths (bath per coupon) of human plasma for 4.5 hours to allow elution of the drug into the plasma. After 4.5 hours, the coupons were removed from the plasma baths, rinsed in deionized water and vacuum dried. Weight measurements were made at the following stages in the process: 1) pre-deposition clean silicon coupon weight; 2) following deposition and drying, weight of coupon plus deposited drug; 3) post-irradiation weight; and 4) post plasma-elution and vacuum drying weight. Thus for each coupon the following information is available: 1) initial weight of the deposited drug load on each coupon; 2) the weight of drug lost during irradiation of each coupon; and 3) the weight of drug lost during plasma elution for each coupon. For each irradiated coupon it was confirmed that drug loss during irradiation was negligible. Drug loss during elution in human plasma is shown in Table 1. The groups were as follows: Control Group—no irradiation was performed; Group 1 —irradiated with a Neutral Beam derived from a GCIB accelerated with a V_(Acc) of 30 kV. The Group 1 irradiated beam energy dose was equivalent to that of a 30 kV accelerated, 5×10¹⁴ gas cluster ion per cm² dose (energy equivalence determined by beam thermal energy flux sensor); Group 2—irradiated with a Neutral Beam derived from a GCIB accelerated with a V_(Acc) of 30 kV. The Group 2 irradiated beam energy dose was equivalent to that of a 30 kV accelerated, 1×10¹⁴ gas cluster ion per cm² dose (energy equivalence determined by beam thermal energy flux sensor); and Group 3—irradiated with a Neutral Beam derived from a GCIB accelerated with a V_(Acc) of 25 kV. The Group 3 irradiated beam energy dose was equivalent to that of a 25 kV accelerated, 5×10¹⁴ gas cluster ion per cm² dose (energy equivalence determined by beam thermal energy flux sensor).

TABLE 1 Group 1 Group 2 Group 3 Group [5 × 10^(14]) [1 × 10¹⁴] [5 × 10¹⁴] [Dose] Control {30 kV} {30 kV} {25 kV} {V_(Acc)} Start Elution Elution Start Elution Elution Start Elution Start Elution Elution Coupon Load Loss Loss Load Loss Loss Load Loss Loss Load Loss Loss # (μg) (μg) % (μg) (μg) % (μg) (μg) % (μg) (μg) % 1 83 60 72 88 4 5 93 10 11 88 — 0 2 87 55 63 100 7 7 102 16 16 82 5 6 3 88 61 69 83 2 2 81 35 43 93 1 1 4 96 72 75 — — — 93 7 8 84 3 4 Mean 89 62 70 90 4 5 92 17 19 87 2 3 σ 5 7 9 3 9 13 5 2 p value 0.00048 0.014 0.00003

Table 1 shows that for every case of Neutral Beam irradiation (Groups 1 through 3), the drug lost during a 4.5-hour elution into human plasma was much lower than for the un-irradiated Control Group. This indicates that the Neutral Beam irradiation results in better drug adhesion and/or reduced elution rate as compared to the un-irradiated drug. The p values (heterogeneous unpaired T-test) indicate that for each of the Neutral Beam irradiated Groups 1 through 3, relative to the Control Group, the difference in the drug retention following elution in human plasma was statistically significant.

FIGS. 15A through 15C show the comparative effects of full beam (charged plus uncharged components) and charge separated beam on a single crystal silicon wafer as may be typically employed in semiconductor applications. The silicon substrate had an initial native oxide layer of approximately 1.3 nm. In separate instances, the silicon substrate was processed using a full GCIB (charged and neutral components), a Neutral Beam derived from a GCIB (charged components removed from the beam by deflection), and a charged cluster beam comprising only the charged components of a GCIB following their separation from the neutral components. All three conditions were derived from the same initial GCIB conditions, a 30 kV accelerated GCIB formed from a mixture of 98% Ar with 2% O₂. For each of the three beams, irradiated doses were matched to the total energy carried by the full beam (charged plus neutral) at an ion dose of 2×10¹⁵ gas cluster ions per cm². Energy flux rates of each beam were measured using a thermal sensor and process durations were adjusted to ensure that each sample received the same total thermal energy dose equivalent to that of the full (charged plus neutral) GCIB. The three samples were evaluated by sectioning followed by imaging by transmission electron microscopy (TEM).

FIG. 15A is a TEM image 1000 of a section of a silicon substrate irradiated by the full GCIB (charged and neutral beam components). The irradiation was incident on the silicon substrate from the direction of the top of the image toward the bottom of the image. Prior to sectioning for TEM imaging, the top surface (irradiated surface) of the silicon substrate was coated with an epoxy overcoat to facilitate the sectioning operation and to avoid damage to the substrate during the sectioning process. In the TEM image 1000, the epoxy overcoat 1006 is seen at the top of the image. The irradiation formed an amorphous region 1004 comprising silicon and oxygen having a minimum thickness of approximately 4.6 nm. A rough interface 1008 having a peak-to-peak variation of approximately 4.8 nm was formed between the amorphous region 1004 and the underlying single crystalline silicon 1002, as a result of the irradiation process.

FIG. 15B is a TEM image 1020 of a section of a silicon substrate irradiated by the separated charged component of the GCIB (charged portion only). The irradiation was incident on the silicon substrate from the direction of the top of the image toward the bottom of the image. Prior to sectioning for TEM imaging, the top surface (irradiated surface) of the silicon substrate was coated with an epoxy overcoat to facilitate the sectioning operation and to avoid damage to the substrate during the sectioning process. In the TEM image 1020, the epoxy overcoat 1026 is seen at the top of the image. The irradiation formed an amorphous region 1024 comprising silicon and oxygen having a minimum thickness of approximately 10.6 nm. A rough interface 1028 having a peak-to-peak variation of approximately 5.9 nm was formed between the amorphous region 1024 and the underlying single crystalline silicon 1022, as a result of the irradiation process.

FIG. 15C is a TEM image 1040 of a section of a silicon substrate irradiated by the neutral portion (charged components separated by deflection and discarded). The irradiation was incident on the silicon substrate from the direction of the top of the image toward the bottom of the image. Prior to sectioning for TEM imaging, the top surface (irradiated surface) of the silicon substrate was coated with an epoxy overcoat to facilitate the sectioning operation and to avoid damage to the substrate during the sectioning process. In the TEM image 1040, the epoxy overcoat 1046 is seen at the top of the image. The irradiation formed an amorphous region 1044 comprising silicon and oxygen having a substantially uniform thickness of approximately 3.0 nm. A smooth interface 1048 having a peak-to-peak variation on an atomic scale was formed between the amorphous region 1044 and the underlying single crystalline silicon 1042, as a result of the irradiation process.

The results of processing shown in FIGS. 15A through 15C indicate that in semiconductor applications, the use of an accelerated Neutral Beam derived from accelerated GCIB by charge separation results in superior interfaces between the irradiation processed and unprocessed regions as compared to either a full GCIB or only the charged portion of a GCIB. The data also shows that a smooth uniform oxide film can be formed on silicon using a Neutral Beam derived from a GCIB and that such film is free of the rough interface often associated with the use of conventional GCIB. Without wishing to be bound to a particular theory, it is believed that the improvement likely results from the elimination of intermediate size clusters or from the elimination of all or most clusters from the beam.

FIG. 16 is a graph 1060 showing results of secondary ion mass spectrometry

(SIMS) depth profile measurement of a shallow boron implantation in a silicon substrate preformed using a Neutral Beam according to an embodiment the invention. The graph plots boron concentration 1062 measured in boron atoms/cc (atoms/cm³) as a function of depth measured in nm. Using apparatus similar to that shown in FIG. 4, a 30 kV accelerated GCIB was formed from a mixture of 99% Ar with 1% diborane (B₂H₆). Stagnation chamber pressure was 80 psi (5.5×10⁵ pascal), nozzle flow was 200 standard cm³/minute (3.3 standard cm³/sec). Full beam current (charged plus neutral components prior to separation by deflection was approximately 0.55 microA (μA). The pressure in the beam path was maintained at approximately 6.9×10⁻⁵ ton (9.2×10⁻³ pascal) and the background gas forming that pressure was essentially argon/diborane. The argon/diborane gas target thickness for the region between the accelerator and the workpiece was approximately 2.23×10¹⁴ argon/diborane gas monomers/cm², and the accelerated Neutral Beam was observed to consist essentially of fully dissociated neutral monomers at the target. Using electrostatic deflection, all charged particles were deflected away from the beam axis and out of the beam, forming the essentially fully dissociated Neutral Beam. Thus the Neutral Beam was an accelerated monomer neutral argon/diborane beam. Dosimetry was done using a thermal sensor to calibrate the total Neutral Beam dose delivered to the silicon substrate such that a Neutral Beam deposited energy equivalent to that energy which would be deposited by a 6.3×10¹⁴ gas cluster ions/cm² irradiation dose by an accelerated (30 kV) GCIB including both the charged and uncharged particles (without neutralization by charge separation). The depth profile shown in FIG. 16 indicates that the Neutral Beam boron ion implantation resulting from using a Neutral Beam derived from a GCIB, results in a very shallow boron implantation. The junction depth estimated from the 10¹⁸ boron atoms/cm³ concentration depth occurs at about 12 nm depth, a very shallow junction. Integrating the boron dose over depth indicates an areal density of approximately 7.94×10¹⁴ boron atoms/cm².

FIG. 17 is a TEM image 1100 of a section of a silicon substrate irradiated by the neutral portion (charged components separated by deflection and discarded) derived from a GCIB. Using apparatus similar to that shown in FIG. 4, a 30 kV accelerated GCIB was formed from a mixture of 99% Ar with 1% diborane (B₂H₆). Stagnation chamber pressure was 88 psi (6.05×10⁵ pascal), nozzle flow was 200 standard cm³/minute (3.3 standard cm³/sec). Full beam current (charged plus neutral components prior to separation by deflection was approximately 0.55 microA (μA). The pressure in the beam path was maintained at approximately 6.8×10⁻⁵ torr (9.07×10⁻³ pascal) and the background gas forming that pressure was essentially argon/diborane. The argon/diborane gas target thickness for the region between the accelerator exit aperture and the workpiece was therefore approximately 2.2×10¹⁴ argon/diborane gas monomers/cm², and the accelerated Neutral Beam was observed to consist essentially of fully dissociated neutral monomers at the target. Using electrostatic deflection all charged particles were deflected away from the beam axis and out of the beam, forming a Neutral Beam, which was essentially fully dissociated. Thus the Neutral Beam was an accelerated monomer neutral argon/diborane beam. Dosimetry was done using a thermal sensor to calibrate the total Neutral Beam dose delivered to the silicon substrate such that a Neutral Beam deposited energy equivalent to that energy which would be deposited by a 1.8×10¹⁴ gas cluster ions/cm² irradiation dose by an accelerated (30 kV) GCIB including both the charged and uncharged particles (without neutralization by charge separation). The irradiation was incident on the silicon substrate from the direction of the top of the image toward the bottom of the image. Prior to sectioning for TEM imaging, the top surface (irradiated surface) of the silicon substrate was coated with an epoxy overcoat to facilitate the sectioning operation and to avoid damage to the substrate during the sectioning process. Referring again to FIG. 17, in the TEM image 1100, the epoxy overcoat 1106 is seen at the top of the image. The irradiation formed an amorphous region 1104 comprising silicon and boron having a substantially uniform thickness of approximately 1.9 nm. A smooth interface 1108 having a peak-to-peak variation on an atomic scale was formed between the amorphous region 1104 and the underlying single crystalline silicon 1102, as a result of the irradiation process. Prior art GCIB irradiation of semiconductor materials for introducing dopants, strain inducing species, etc. are known to form rougher interfaces between the processed film and the underlying substrate, similar to the interface 1008 shown in FIG. 15A. It is shown that diborane can be employed to effectively dope a semiconductor with boron, with a high quality interface between the doped film and the underlying substrate. By using other gases containing other dopant and/or lattice-straining species, species for increasing the solid solubility limit of a dopant, or species for promoting surface amorphization, high quality films with superior interfaces between film and substrate may be obtained as compared to conventional GCIB technology, where the presence of intermediate-sized cluster ions in the beam may result in a rough interface. Some dopant-containing gases that may be employed alone or in mixtures for introducing dopants are, diborane (B₂H₆), boron trifluoride (BF₃), phosphine (PH₃), phosphorous pentafluoride (PF₅), arsine (AsH₃), and arsenic pentafluoride (AsF₅), as examples without limitation, may be employed for incorporating dopant atoms into gas clusters. Some gases that may be employed alone or in mixtures for introducing lattice-straining species are germane (GeH₄), germanium tetrafluoride (GeF₄), silane (SiH₄), silicon tetrafluoride (SiF₄), methane, (CH₄). Some gases that may be employed alone or in mixtures for promoting amorphization are, without limitation, argon (Ar), germane (GeH₄), germanium tetrafluoride (GeF₄), and fluorine (F₂). Some gases that may be employed alone or in mixtures for promoting dopant solubility are germane (GeH₄) and germanium tetrafluoride (GeF₄). Dopant-containing gases, gases containing lattice-straining species, gases containing amorphizing species, and/or gases containing species for improving dopant solubility (and optionally inert or other gases) may be employed in mixtures for simultaneous formation of combinations of benefits by the accelerated Neutral Beam process. In FIG. 17, the lead line connecting the numeric designator 1108 to its object changes color to maintain contrast on regions in the figure having differing backgrounds.

FIG. 18 illustrates a depth profile measurement graph 1200 obtained after using an accelerated Neutral Beam derived from a GCIB to etch a silicon dioxide (SiO₂) film on a silicon substrate and to etch the silicon substrate. Using apparatus similar to that shown in FIG. 4, a 30 kV accelerated GCIB was formed using argon. Stagnation chamber pressure was 28 psi (1.93×10⁵ pascal), nozzle flow was 200 standard cm³/minute (3.3 standard cm³/sec). Full beam current (charged plus neutral components prior to separation by deflection was approximately 0.50 microA (μA). The argon gas target thickness for the region between the accelerator and the workpiece was approximately 1.49×10¹⁴ argon gas monomers/cm², and the accelerated Neutral Beam was observed to consist essentially of fully dissociated neutral monomers at the target. Using electrostatic deflection all charged particles were deflected away from the beam axis and out of the beam, forming a Neutral Beam. Thus the Neutral Beam was essentially an accelerated neutral argon monomer beam. Dosimetry was done using a thermal sensor to calibrate the total Neutral Beam dose delivered to the silicon substrate such that a Neutral Beam deposited energy equivalent to that energy which would be deposited by a 2.16×10¹⁶ gas cluster ions/cm² irradiation dose by an accelerated (30 kV) GCIB including both the charged and uncharged particles (without neutralization by charge separation). A silicon dioxide (SiO₂) film (approximately 0.5 micron [μm] thick) on a silicon substrate was partially masked with a narrow (approximately 0.7 mm wide) strip of polyimide film tape and then irradiated with the accelerated Neutral Beam. Following the irradiation the polyimide tape was removed. Referring again to FIG. 18, the depth profile measurement graph 1200 was generated using a TENCOR Alpha-Step 250 profilometer to measure the step profile, in a direction along the surface of the SiO₂ film (on silicon substrate) and across the region masked by the polyimide film tape, due to the etching resulting from the accelerated Neutral Beam. Plateau 1202 represents the unetched surface of the SiO₂ film beneath the polyimide film (after film removal and cleaning), while the regions 1204 represent the etched portion. The accelerated Neutral Beam produced an etch depth of approximately 2.4 microns (μm), etching all the way through the 0.5 micron SiO₂ film and an additional 1.9 microns into the underlying crystalline silicon substrate, producing the step shown in depth profile measurement graph 1200. Argon and other inert gases may be used as source gases to etch by physical means. By using a reactive source gas or using a source gas incorporating a reactive gas in a mixture, reactive etching can also be performed using a Neutral Beam. Typical reactive gases that may be used alone or in mixture with inert gases are (without limitation) oxygen (O₂), carbon dioxide (CO₂), nitrogen (N₂), ammonia (NH₃), fluorine (F₂), chlorine (Cl₂), sulfur hexafluoride (SF₆), tetrafluoromethane (CF₄), and other condensable halogen-containing gases.

FIGS. 19A and 19B are TEM images illustrating production of amorphous layers in crystalline semiconductor material by irradiating with accelerated Neutral Beams derived from GCIBs. Prior to sectioning for TEM imaging, the top surface of each sample was coated with an epoxy overcoat to facilitate the sectioning operation and to avoid damage to the surface during the sectioning process. Native oxide forms spontaneously in air or water when bare silicon is exposed.

FIG. 19A is a TEM image 1220 of a section of a silicon substrate with a film of native SiO₂. In the TEM image 1220, the epoxy overcoat 1226 is seen at the top of the image. A thin (approximately 1.3 nm) native oxide film 1224 is seen on the underlying silicon substrate 1222.

FIG. 19B is a TEM image 1240 showing results of irradiation of a silicon substrate by an accelerated argon Neutral Beam derived from a GCIB. A silicon wafer having a native oxide film similar to that shown in FIG. 19A was cleaned in 1% aqueous solution of hydrofluoric acid to remove the native oxide. The cleaned silicon substrate was irradiated using a Neutral Beam derived from a 30 kV accelerated GCIB (charged components removed from the beam by deflection) formed from argon. The irradiated dose was matched in energy to the total energy carried by a full beam (charged plus neutral) at an ion dose of 5×10¹⁴ gas-cluster ions per cm² by using a thermal sensor to match the total energy deposited by the Neutral Beam to that of the full 5×10¹⁴ gas-cluster ions per cm² beam. Referring again to FIG. 19B, the TEM image 1240 shows the epoxy overcoat 1246, a 2.1 nm thick amorphous film 1244 in the surface of the silicon formed by the accelerated Neutral Beam irradiation, overlying the crystalline silicon substrate material 1242. A smooth interface 1248 having a peak-to-peak variation on an atomic scale was formed between the amorphous film 1244 and the underlying crystalline silicon material 1242, as a result of the irradiation process. This shows that the noble gas, argon (Ar), may be employed to form an amorphous layer in a crystalline semiconductor material. Some other gases (without limitation) that may be used to form amorphous layers by employing them in formation of accelerated Neutral Beams for embodiments of the invention include, xenon (Xe), germane (GeH₄), and germanium tetrafluoride (GeF₄). Such source gases may be used alone or in mixtures with argon or other noble gases. In FIG. 19B, the lead line connecting the numeric designator 1248 to its object changes color to maintain contrast on regions in the figure having differing backgrounds.

FIGS. 20A and 20B are TEM images illustrating the growth of an oxide film on silicon by the use of accelerated Neutral Beams derived from GCIBs. Prior to sectioning for TEM imaging, the top surface of each sample was coated with an epoxy to facilitate the sectioning operation and to avoid damage to the surface during the sectioning process.

FIG. 20A is a TEM image 1260 showing results of irradiation of a silicon substrate by an accelerated Neutral Beam derived from a GCIB. A silicon wafer having a native oxide film similar to that shown in FIG. 19A was cleaned in 1% aqueous solution of hydrofluoric acid to remove the native oxide. The cleaned, bare silicon substrate was then irradiated using a Neutral Beam derived from a 30 kV accelerated GCIB (charged components removed from the beam by deflection) formed from a source gas mixture of 98% Ar with 2% O₂. The irradiated Neutral Beam dose was energetically equivalent (energy equivalence determined by beam thermal energy flux sensor) to a 30 kV accelerated GCIB at an ion dose of 2.4×10¹³ gas cluster ions per cm². Referring again to FIG. 20A, the TEM image 1260 shows the epoxy overcoat 1266, a 2 nm thick oxide film 1264 in the surface of the silicon formed by the accelerated Neutral Beam irradiation, overlying the crystalline silicon substrate material 1262. A smooth interface 1268 having a peak-to-peak variation on an atomic scale was formed between the oxide film 1264 and the underlying crystalline silicon material 1262, as a result of the irradiation process. In FIG. 20A, the lead line connecting the numeric designator 1268 to its object changes color to maintain contrast on regions in the figure having differing backgrounds.

FIG. 20B is a TEM image 1280 showing results of irradiation of a silicon substrate by an accelerated Neutral Beam derived from a GCIB. A silicon wafer having a native oxide film similar to that shown in FIG. 19A was cleaned in 1% aqueous solution of hydrofluoric acid to remove the native oxide. The cleaned, bare silicon substrate was then irradiated using a Neutral Beam derived from a 30 kV accelerated GCIB (charged components removed from the beam by deflection) formed from a source gas mixture of 98% Ar with 2% O₂. The irradiated Neutral Beam dose was energetically equivalent (energy equivalence determined by beam thermal energy flux sensor) to a 30 kV accelerated GCIB at an ion dose of 4.7×10¹⁴ gas cluster ions per cm². Referring again to FIG. 20B, the TEM image 1280 shows the epoxy overcoat 1286, a 3.3 nm thick oxide film 1284 in the surface of the silicon formed by the accelerated Neutral Beam irradiation, overlying the crystalline silicon substrate material 1282. A smooth interface 1288 having a peak-to-peak variation on an atomic scale was formed between the oxide film 1284 and the underlying crystalline silicon material 1282, as a result of the irradiation process. This shows that a Neutral Beam comprising oxygen may be employed to form an oxide layer at the surface of a semiconductor material. The thickness of the film grown may be varied by varying the irradiated dose. By using source gases comprising other reactive species in forming the accelerated Neutral Beam, other types of films may be grown on semiconductor or other surfaces, for examples (without limitation), oxygen (O₂), nitrogen (N₂), or ammonia (NH₃), alone or in mixture with argon (Ar) or other noble gas may be employed. In FIG. 20B, the lead line connecting the numeric designator 1288 to its object changes color to maintain contrast on regions in the figure having differing backgrounds.

FIG. 21 illustrates a depth profile measurement graph 1300 obtained after using an accelerated Neutral Beam derived from a GCIB to deposit a diamond-like carbon film on a silicon substrate. Using apparatus similar to that shown in FIG. 4, a 30 kV accelerated GCIB was formed using a source gas mixture of 10% methane (CH₄) with 90% argon. The accelerated Neutral Beam was observed to consist essentially of fully dissociated neutral monomers at the target. Using electrostatic deflection all charged particles were deflected away from the beam axis and out of the beam, forming a neutral methane/argon beam. Thus the Neutral Beam was essentially an accelerated neutral methane/argon monomer beam. Dosimetry was done using a thermal sensor to calibrate the total Neutral Beam delivered to the silicon substrate such that the Neutral Beam deposited energy equivalent to that energy which would be deposited by a 2.8 microA gas cluster ions/cm² irradiation dose by an accelerated (30 kV) GCIB, including both the charged and uncharged particles (without neutralization by charge separation). A silicon substrate was partially masked with a narrow (approximately 1 mm wide) strip of polyimide film tape and then the substrate and mask were irradiated with the accelerated Neutral Beam for 30 minutes, depositing a diamond-like carbon film. Following irradiation the mask was removed. Referring again to FIG. 21, the depth profile measurement graph 1300 was generated using a TENCOR Alpha-Step 250 profilometer to measure the step profile, in a direction along the surface of the silicon substrate and across the region masked by the polyimide film tape, due to the deposition resulting from the accelerated Neutral Beam. Flat region 1302 represents the original surface of the silicon substrate beneath the polyimide film (after film removal and cleaning), while the regions 1304 represent the deposited diamond-like carbon portion. The accelerated Neutral Beam produced a deposition thickness of approximately 2.2 microns (um), producing the step shown in depth profile measurement graph 1300. The deposition rate was approximately 0.45 nm/sec for each microA/cm² of GCIB current (the energetic equivalent, as determined by thermal sensor as mentioned above in this paragraph). In other tests, 5% mixture and 7.5% mixtures of CH₄ in argon, gave similar results, but with lower deposition rates resulting from lower CH₄ percentage in the source gas. Selection of gas mixture and dose permit repeatable deposition of films with predetermined thicknesses. CH₄, alone or in mixture with argon or other noble gas is an effective source gas for depositing carbon using an accelerated neutral monomer beam. Other typical gases that may be used alone or in mixture with inert gases for film deposition using accelerated neutral monomer beams are (without limitation) germane (GeH₄), germanium tetrafluoride (GeF₄), silane (SiH₄), and silicon tetrafluoride (SiF₄).

FIG. 22 shows a typical map 1320 resulting from an atomic force microscope (AFM) evaluation a 500 nm by 500 nm region of the surface of a conventionally cleaned and polished sample of a borosilicate optical glass (Corning type 0211) of a type commonly employed in applications such as optical windows, display and/or touch-screen substrates, microscopy slides and coverslips, filters, and the like. The surface has an average roughness, R_(A), equal to 0.27 nm and exhibits numerous asperities 1322 having a height on the order of a few nm. Total peak-to-valley deviations are on the order of about 4 nm or more.

Processing such a surface using an essentially fully dissociated Neutral Beam derived from an accelerated GCIB results in considerable smoothing and planarization, and reduces the total peak-to-valley deviation. A conventionally cleaned and polished sample of Corning type 0211 optical glass was irradiated using a Neutral Beam derived from a 30 kV accelerated GCIB (charged components removed from the beam by deflection) formed from an Argon source gas. The irradiated Neutral Beam dose was energetically equivalent (energy equivalence determined by beam thermal energy flux sensor) to a 30 kV accelerated GCIB at an ion dose of 1×10¹⁴ gas cluster ions per cm².

FIG. 23 shows a map 1340 resulting from an AFM evaluation a 500 nm by 500 nm region of the surface of the Neutral Beam irradiated glass. The surface has an average roughness, R_(A), equal to 0.13 nm, approximately half the roughness of the unirradiated material. The surface is essentially free of asperities. Total peak-to-valley deviations are on the order of about 2 nm, approximately half that of the unirradiated optical surface.

The use of an accelerated Neutral Beam derived from an accelerated GCIB by separation of charged components from uncharged components is shown to be capable of numerous applications in the field of semiconductor processing, with an added benefit that the interface between the layer formed by the irradiation and the underlying semiconductor is extremely smooth and superior to results obtained by conventional GCIB irradiation.

Another optical application that benefits from GCIB or Neutral Beam processing is related to the problem of adhering an optical film onto an optical substrate. Optical devices are commonly improved by coating them with various thin films to enhance or improve performance. Such optical films may be employed as protective coatings, anti-reflection coatings, high reflection coatings, or in combinations to produce dichoric thin film optical filters. The coatings may be thin metal films (for examples aluminum or gold), dielectric films (for examples magnesium fluoride, calcium fluoride, or metal oxides), or may be conductive films to enhance anti-static properties or to serve as electrodes for display or touch sensitive structures. Such thin film coatings are often deposited using physical vapor deposition (PVD) techniques or other conventional techniques suitable for the purpose. A common problem is that such films often do not form a strong interface with the substrate or subsequent layers and thus may not be as well adhered as is desirable. A problem arises because the coatings applied by PVD and other conventional techniques often do not form strong bonds to the substrate materials because of their dissimilarity with the substrate materials. GCIB or Neutral Beam processing may be employed to produce thin film coatings on optical substrates (onto optical devices or over other optical coatings) that are much more strongly adhered than coatings applied by the conventional techniques. To achieve a higher adhesion performance, a GCIB or Neutral Beam may be used to convert an initial seed coating to a strongly integrated interface layer with the substrate, and then form the final coating to the desired thickness on the interface layer. Although both GCIB and Neutral Beam may be employed in many circumstances, in the cases where either the substrate or the coating is a dielectric or low conductivity material, the Neutral Beam is preferred because of the aforementioned advantages it has for avoiding damage due to the charge transport inherent in ion beam processing. Both GCIB and Neutral Beam processing achieve an enhanced adhesion of the coating without significant subsurface damage as often occurs with conventional monomer ion beams.

FIGS. 24A through 24D are schematics illustrating steps in embodiments of the invention for the formation of strongly adhered optical coatings on optical substrates using GCIB or Neutral Beam techniques. FIG. 24A is a schematic 1400 showing an optical substrate 1402, having a very thin film coating of an optical coating material, 1404 having been previously applied by a conventional technique such as PVD. There is an interface 1406 between the optical coating material 1404 and the optical substrate 1402 that has conventional adhesion properties (which may be inadequate for the intended application). The thickness of the substrate 1402 and the optical coating material 1404 are not necessarily shown to scale. GCIBs and Neutral Beams have penetration characteristics dependent on the beam source materials, the beam acceleration potentials used, and the range of sizes of any clusters present in the beam (though in a fully dissociated Neutral Beam, clusters are not present). Dissociated Neutral Beams may, for example, have penetration depths into a typical optical coating material on the order of from about 1 to 3 nm, while GCIB and Neutral Beams containing clusters may have penetration depths on the order of from about 2 to 20 nm (all dependent on the coating material and beam parameters.) In the method of this embodiment of the invention the thickness of the optical coating material 1404 is chosen so that a practical beam typical parameters will penetrate the entire thickness of the optical coating material 1404 and also penetrate a short distance (on the order of 1 to a few nm) into the optical substrate 1402.

FIG. 24B is a schematic 1410 showing irradiation of the optical coating material 1404 with a beam 1412, which is a GCIB or a Neutral Beam. The beam 1412 characteristics are selected in conjunction with the thickness of the optical coating material 1404 so that it is assured that at least a fraction of the particles in the beam 1412 incident on the optical coating material 1404 penetrate it entirely. Those that penetrate, pass through the conventional interface 1406, and into the optical substrate 1402 for a distance on the order of from about 1 to a few nm. The irradiated GCIB dose or Neutral Beam dose is for example at least 5×10¹³ ions per cm² of a for example 30 kV accelerated GCIB, or in the case of a Neutral Beam, energetically equivalent (energy equivalence determined by beam thermal energy flux sensor) to a for example 30 kV accelerated GCIB having an ion dose of at least 5×10¹³ gas cluster ions per cm².

FIG. 24C is a schematic 1420 showing the structure which results from the irradiation described above. Interaction of the beam with the thin film of optical coating material 1404 drives atoms from the optical coating material 1404 into the optical substrate 1402, forming a mixture region 1422, wherein the atoms of the optical coating material 1404 and the optical substrate 1402 are intimately mixed, with a concentration gradient of optical coating material atoms being higher in the upper regions of the mixture region and approaching zero in the lower regions of the mixture region. The similar atoms in the upper regions of the mixture region 1422 facilitate a strong bond with the atoms of the optical coating material 1404 resulting in the optical coating material 1404 being much more strongly adhered to the optical substrate than in the case of the conventional interface 1406 (shown in FIG. 4A). The thickness of the optical coating material 1404, which is necessarily limited in thickness to allow penetration of the beam to form the mixture region 1422, may be too thin for the desired optical coating properties, in such case, a subsequent deposition of additional optical coating material is required to create the desired optical coating properties.

FIG. 24D is a schematic 1430 illustrating an additional deposited layer of optical coating material 1432 to increase the net thickness of optical coating material 1404 plus optical coating material 1432 to the thickness necessary for the desired optical effect. Material 1404 and material 1432 are commonly the same material, though they could be different materials, provided the two materials form a strong adhesion between themselves. In one case, the material 1404 may be dissimilar to both the optical substrate material and the upper material 1432, but the material 1404 may be chosen to bond chemically with both the substrate and the upper material, whereas the upper material and the optical substrate may have no inherent affinity for each other. In the case of the two materials (material 1404 and material 1432) being the same, the similarity of atoms typically results in much stronger adhesion between the two layers than occurs for the conventional interface 1406 (which was shown in FIG. 24A.)

A further application that benefits from GCIB or Neutral Beam processing is related to the problem of atmospheric degradation of materials. For example optical and other devices commonly employ materials that have highly desirable optical characteristics, but which suffer from also having characteristics that make them susceptible to degradation when exposed to ordinary atmospheric conditions. This limits their usefulness or useful service lifetime or useful shelf life when it is not practical to avoid atmospheric exposure. Such materials may degrade due to surface oxidation, absorption of atmospheric moisture, or due to other reaction of the material's surfaces at the atmospheric interface. A specific example is the material, lithium triborate (LBO), LiB₃O₅, which is a preferred material for many non-linear optics (NLO) applications. In NLO applications, LBO often outperforms other available materials, but suffers from the disadvantage that it is hygroscopic and is degraded by absorption of moisture from the atmosphere or other sources. This limits the effective lifetime of the material in many applications, or even in other applications where limited atmospheric shelf-life causes degradation before the material is placed into service. Additive surface coatings have conventionally been employed reduce the rate of moisture absorption by providing a moisture barrier. However these are not always as effective as may be required, and especially in the case of applications where the optical power density is high (e.g. laser applications), coatings may delaminate or otherwise degrade and loose effectiveness with time. As described hereinabove, the adhesion of such coatings may be improved by employing the GCIB and accelerated Neutral Beam techniques previously disclosed for improving film adhesion. However, GCIB or accelerated Neutral Beam irradiation may also be employed to form a thin barrier that reduces surface reactivity and/or moisture susceptibility. The irradiation-formed barrier may be used in combination with subsequently applied conventional barrier coatings, if desired. Although both GCIB and Neutral Beam may be employed in many circumstances, the material treated is either a dielectric or low conductivity material, the Neutral Beam is preferred because of the aforementioned advantages it has for avoiding damage due to the charge transport inherent in ion beam processing. LBO surfaces deteriorate rapidly when exposed directly to typical ambient atmospheric conditions. Accelerated Neutral Beam irradiation of LBO surfaces significantly delays such deterioration.

FIGS. 25A and 25B are atomic force micrograph maps of surfaces of an untreated LBO optical component showing degradation due to atmospheric exposure.

FIG. 25A shows a surface of an uncoated LBO optical component that has been (for less than one hour) exposed to a typical ambient laboratory atmosphere in a conventionally air conditioned building. The map shows a typical one micron by one micron square region of the crystal. The linear trough-like features are residual scratches in the conventionally polished surface. Numerous elevated bumps have appeared, indicative of onset of surface degradation due to atmospheric exposure of the hygroscopic LBO material. The surface exhibits an average roughness, Ra, of approximately 0.30 nm.

FIG. 25B shows a typical one micron by one micron square region of the same piece of LBO material after 100 hours of exposure to the same ambient laboratory atmosphere. The surface degradation is seen to have progressed substantially—average roughness, Ra, is increased to approximately 3.58 nm, due to the increased areas and heights of the bumps growing on the surface.

FIGS. 26A and 26B are atomic force micrograph maps of surfaces of an LBO optical component treated using an accelerated Neutral Beam derived from a GCIB, with resulting reduced degradation due to atmospheric exposure.

FIG. 26A shows a surface of the same piece of uncoated LBO optical component that was shown above in FIG. 25A. After brief (for less than one hour) exposure to ambient laboratory atmosphere in a conventionally air conditioned building, a portion of the surface was processed with accelerated Neutral Beam irradiation. Following the irradiation step, the atomic force microscope image of part of the irradiated portion shown in FIG. 26A was measured. The map shows a typical one micron by one micron square region of the irradiated portion of the crystal immediately after irradiation. The linear trough-like scratches are no longer apparent and the surface exhibits an average roughness, Ra, of approximately 0.26 nm. The irradiated portion of the surface was irradiated using a Neutral Beam derived from an argon GCIB accelerated using V_(Acc) of 30 kV. The Neutral Beam was irradiated with a neutral atom dose of 5×10¹⁸ argon atoms per cm². Other experiments have shown that a neutral atom dose of as low as 2.5×10¹⁷ argon atoms per cm² is effective (alternatively, effective GCIB doses have similar acceleration and a combination of cluster ion sizes and dose that provide a similar dose of argon atoms).

FIG. 26B shows a typical one micron by one micron square region of the same piece of LBO material after 100 hours of continued exposure to the same ambient laboratory atmosphere. The surface degradation has progressed very little—average roughness, Ra, is approximately 0.29 nm. The Neutral Beam irradiation has resulted in a shallow surface modification that functions as a barrier to moisture absorption and perhaps other forms of degradation, extending the functionally useful lifetime of the hygroscopic LBO optical material. At the end of 100 hours of atmospheric exposure the irradiated surface appears of equal or better quality than that of the original material after just one hour of atmospheric exposure.

A further application that benefits from Neutral Beam processing is related to the formation of a SiC or SiCX (0.05<X<3) layer on a silicon substrate for providing a surface that is harder, that is more heat resistant, that is less damage prone, that is more refractory, that has improved chemical properties, that has different lattice constants, that may serve as a base for subsequent layer growth, that may serve as a substrate for deposition of subsequent material (lattice matching or improved bonding), to serve as a silicon-carbide semiconductor layer on a silicon substrate or to otherwise improve the silicon substrate. FIGS. 24A through 24D are schematics illustrating steps in embodiments of the invention for the formation of strongly adhered optical coatings on optical substrates using GCIB or Neutral Beam techniques. FIG. 27A is a schematic 1500 showing a silicon substrate 1502, which may be a single crystal silicon substrate and may be of high purity as is used for semiconductor manufacturing. The thickness of the silicon substrate 1502 is not necessarily shown to scale. Neutral Beams have penetration characteristics dependent on the beam source materials, the beam acceleration potentials used, and the range of sizes of any clusters present in the beam (though in a fully dissociated Neutral Beam, clusters are not present). Dissociated Neutral Beams may, for example, have penetration depths into a typical optical coating material on the order of from about 1 to 3 nm, while Neutral Beams containing clusters may have penetration depths on the order of from about 2 to 20 nm (dependent on the target material and beam parameters.)

FIG. 27B is a schematic 1510 showing irradiation of the silicon substrate 1502 with a beam 1512, which is a Neutral Beam (preferably a Dissociated Neutral Beam. The beam 1512 characteristics (including acceleration potential and dose and source gas) are selected so that it penetrates the silicon substrate 1502 a predetermined desired depth so that it implants a quantity of carbon atoms appropriate to make the C:Si ratio in the implanted region between about 0.05 to about 3 carbon atoms per silicon atom. A carbon-containing source gas (preferably methane) is used to provide carbon atoms in the beam. The implantation forms an implanted layer (which may be amorphous) having the desired thickness and carbon:silicon atomic ratio. The preferred range for irradiated Neutral Beam dose and acceleration potential is, for example, about 1×10¹⁴ to about 5×10¹⁶ carbon atoms per cm² (for a beam comprising neutral methane clusters and/or monomers) formed from gas-cluster ions accelerated using 5 to 50 kV acceleration potential prior to forming the Neutral Beam or Dissociated Neutral Beam from the gas-cluster ions.

FIG. 27C is a schematic 1520 showing the structure which results from the irradiation described above. Interaction of the beam with the surface of the silicon substrate 1502 implants carbon and hydrogen atoms into the silicon substrate 1502, forming implanted layer 1522, wherein the atoms of the carbon and the silicon substrate 1502 are mixed. The hydrogen atoms from the beam are volatile and escape the implanted layer, leaving carbon and silicon atoms in the layer. The implanted layer will be disrupted by the carbon atoms and may be amorphous if the carbon: silicon ratio is sufficiently high.

FIG. 27D is a schematic 1530 illustrating the effect of heat treatment (annealing) on the implanted layer 1522 (FIG. 27C) following a heat treating step. The heat treating is preferably in an argon atmosphere or other inert atmosphere using a furnace or radiant heating apparatus capable of providing sufficient temperature-time treatment (according to known techniques) to anneal the implantation damage and move the implanted carbon to lattice substitutional sites. The annealed heat treated layer 1532 is restored to a substantially crystalline form.

Although embodiments of the invention have been described with respect to a hygroscopic LBO optical material, it is understood by the inventors that it is equally applicable to other hygroscopic crystalline materials as may be employed in optical and other applications. For examples hygroscopic thallium-doped sodium iodide crystals and slightly hygroscopic thallium- or sodium-doped cesium iodide crystals are used in gamma ray scintillation spectroscopy and are subject to degradation due to moisture absorption. Such degradation may be delayed or reduced by irradiation. Although the example described above utilized Neutral Beam irradiation of LBO, it is understood by the inventors that GCIB irradiation may also be applied effectively, though Neutral Beam irradiation is considered preferable in the case of materials having low electrical conductivity. It is also understood by the inventors that prior to irradiation to reduce surface degradation of hygroscopic materials, it may be useful to use a pretreatment of GCIB or Neutral beam to smooth the surface and remove existing surface degradation.

Although embodiments of the invention have been described with respect to silicon semiconductor materials, it is understood by the inventors that it is equally applicable to other semiconductor materials including germanium, and compound semiconductors including, without limitation, group III-V and group II-VI and related materials and it is intended that the scope of the invention is intended to include those materials.

It is understood by the inventors that although embodiments of the invention has been shown for exemplary purposes to be useful for processes such a smoothing, etching, film growth, film deposition, amorphization, and doping by using silicon semiconductor wafers, it is understood by the inventors that the benefits of the invention are not limited only to processes done on bare semiconductor surfaces, but are equally useful for processing portions of electrical circuits, electrical devices, optical elements, integrated circuits, micro-electrical mechanical systems (MEMS) devices (and portions thereof) and other devices that are commonly constructed using conventional modern technologies on silicon substrates, other semiconductor substrates, and substrates of other materials, and it is intended that the scope of the invention includes such applications.

Although the benefits of applying the Neutral Beam of the invention for electrical charging-free processing have been described with respect to processing various electrically insulating and/or non-electrically-conductive materials such as insulating drug coatings, dielectric films such as oxides and nitrides, insulating corrosion inhibitor coatings, polymers, organic films, glasses, ceramics, it is understood by the inventors that all materials of poor or low electrical conductivity may benefit from using the Neutral Beam disclosed herein as a substitute for processing with charge transferring processing techniques like ion beams, plasmas, etc., and it is intended that the scope of the invention includes such materials. It is further understood by the inventors that Neutral Beam processing is advantageous not only because of its reduced charging characteristics, but also for processing many materials that are electrically conductive, where other advantages of Neutral Beam processing, especially neutral monomer beam processing, which produces less surface damage, better smoothing, and smoother interfaces between processed and underlying unprocessed regions, even in metals and highly conductive materials. It is intended that the scope of the invention includes processing of such materials.

Although the benefits of applying the Neutral Beam disclosed herein for electrical charging-free processing have been described with respect to processing various insulating and/or non-electrically-conductive materials, it is understood by the inventors that the charge-free Neutral Beam processing benefits apply equally to the processing of electrically conductive, semiconductive, or slightly conductive materials that exist in the form of coatings or layers or other forms overlying insulating layers or disposed upon insulating substrates, wherein the at least slightly conductive materials have no reliable ground connection or other pathway for removing surface charges that may be induced by processing using charge transferring processing techniques. In such cases, charging of the at least slightly conductive materials during processing may produce damage to those materials or to the underlying insulating materials. The charging and damage may be avoided by using the Neutral Beam processing of the invention. It is intended by the inventors that the scope of the invention includes processing of such dissimilar material arrangements where an at least slightly conductive material overlays an insulating material.

Although the benefits of applying the Neutral Beam of the invention for smoothing optical materials have been described with respect to processing Corning type 0211 optical glass, an amorphous material it is understood by the inventors that the charge-free Neutral Beam processing benefits apply equally to the processing other optical materials, amorphous or crystalline, including without limit, glasses, quartz, sapphire, diamond, and other hard, transparent optical materials (either employed as optical elements or as gem [natural or synthetic] materials). It is further understood by the inventors that Neutral Beam processing may be used for also applying optical coatings to such materials and for affecting optical characteristics of such materials, such as the refractive index. It is intended by the inventors that the scope of the invention includes processing of such materials for optical and gem applications.

Although the invention has been described with respect to various embodiments, it should be realized this invention is also capable of a wide variety of further and other embodiments within the spirit and scope of the invention. 

1-17. (canceled)
 18. A silicon substrate, comprising a surface layer of SiC_(x) (0.05<X<3) formed by accelerated and focused Neutral Beam irradiation of a silicon substrate, wherein the Neutral Beam is derived from a gas cluster ion beam comprising carbon atoms, which gas cluster ion beam has had its cluster ions dissociated and charged particles removed, and further wherein a Neutral Beam irradiated surface of the silicon substrate comprises an improved smoothness over comparable gas cluster ion beam irradiation.
 19. The silicon substrate of claim 18, wherein the Neutral Beam consists essentially of neutral monomers and is dosimetry controlled, and further wherein the Neutral Beam irradiated surface comprises uniform improved smoothness over comparable gas cluster ion beam irradiation.
 20. A silicon substrate, comprising a surface layer of SiC_(x) (0.05<X<3) formed by the process of claim 1, wherein the surface layer comprises an improved smoothness over comparable gas cluster ion beam irradiation. 